Altechna Catalog 2013

Laser products catalog 2013

2 / www.altechna.com

Altechna Company Group is a Lithuanian private capital leading company group of international photonic and laser research working since 1996. For 16 years it has been successfully following its mission to create competitive advantage and added value to the customers by innovative solutions in light technologies. See the time-line for the main historic development events of Altechna Group.

Altechna, founded in 1996 as an international photonic and laser company is a reliable

supplier of laser products: general optics, polarization optics, laser and nonlinear crystals, lasers and laser accessories, custom optics, metrology and consulting servicesfor scientific research laboratories by highly qualified physicists. Altechna ensures high quality of all the products as they are thoroughly tested and inspected in its in-house metrology laboratory.

ALTECHNA products:

• Generaloptics;• Polarizationoptics;• Laser&nonlinearcrystals;• Lasers&laseraccessories;• Customoptics;• Metrologyandotherservices.

Mainactivities:

• Tradeandmanufactureoflaserrelatedcomponents;• Designofoptomechanicalassemblies;• Innovativesolutionsforacademicandindustrialcustomers.

About Us

Altechnafounded

First lasermicrofabrication

systems

Associatedcompany

EVANATechnologies

Microlaserlaboratorylaunched

ISO 9001certificate

AssociatedcompanySPRANA

Microfabricationlaboratorylaunched

Associatedcompany ELAS

Metrologylaboratorylaunched

Altechna R&Dfounded

Officialdistributor

of key brands

1996 2004 2005 2006 2007 2008 2009 2010 2011 2012

Our strengths:

• Qualitymanagementsystem ISO9001:2008certification;• Flexiblesupportbyqualifiedphysicistsstaff ;• Productqualityassurancewithin-housemetrologylaboratory;• Multiplelaserrelatedsolutionsfromonehands;• Over10’000laserproductavailableonline;• Directandpromptordershipment.

Acknowledgments:

• In“KnowledgeEconomyCompany2011”awardsAltechnawasacknowledged as the most advanced high-tech company.

• In “Swedish Business Awards 2011” Altechna received MostSustainableGrowthaward.

• Altechnaisthewinnerofthe2011GermanBusinessAwardforits leading technologies and its exemplarymixture of youngandexperiencedemployees.

Memberof :

Certifiedwith

www.altechna.com / 3

Workshop of Photonics®, a daughter company of Altechna, started its activity as a division of Altechna in 2004.ItisaprivatecapitalR&Dbrandin the field of femtosecond laser micromachining.

Workshop of Photonics® is all about laser micromachining. We create instruments and solutions for laser micromachining tasks: from feasibility study to customized optical module and from electronics device to a laser laboratory or laser machine. Our services are targeted both to industry and to academic customers.

Our key services and products:

• Feasibilitystudyonfemtosecondlasermicromachining• Developmentoflaserprocess• Development of custom micro-machining laser systems and

optical modules for industrial or scientific customers• Lasersystemautomationsoftware• Custom electronic andoptomechanic devices for laser based

systems

Our key customer groups:

• Scientificinstitutionsandlaboratories• Business clients andmanufacturers, which need laser micro-

processing tasks in their value chains• Integrators of manufacturing machinery, which supply laser

micro-machining capabilities to their industrial clients

Workshop of Photonics® received “Innovation product” awardin the national contest “Innovation prize 2010” for solar cellprocessing workstation SOLLAS.

www.wophotonics.com

KEyACTIvITyFIELDS

Manufacturing

Laser micromachining

systemsMicrolasers

Spectroscopy

systemsLaser related

devices

Laser related components

Laser opticsCrystals

Lasers andoptomechanics

devices

Distribution

MotionControlScientific cameras

SpectroscopyLaser systems

R&D solutions

Laser micro-machiningSoftware

Laser sourcesOptoelectronics

Quality and measurement

laboratory


MAInR&DPARTnERS

European UnionEuropean UnionSwitz.Switz.

CanadaCanada

USAUSA

MexicoMexico

BrazilBrazil

ArgentinaArgentinaChileChile

IndiaIndiaUAEUAE

NorwayNorway

ByelorussiaByelorussiaUkraineUkraine

RussiaRussia

TunisiaTunisia IsraelIsrael

TurkeyTurkey

South AfricaSouth Africa

JapanJapanKoreaKorea

ChinaChina

TaiwanTaiwan

SingaporeSingapore

New ZealandNew Zealand

AustraliaAustralia


DISTRIBuTORS

REPRESEnTEDCOMPAnIES

China FellesPhotonic

France

AcalBFiFrance

Fibercryst

Germany OptoprimGmbH

India

AvP

ProgressiveMarketers

IISOL

IsraelRoshElectropticsLtd.

Japan

Hikari

Laser Systems

MSquare

Korea

L2K

MJLCrystekInc.

unithinkInc.

Taiwan veego

USA Magic PhotonicsLLC

WeareconstantlylookingforactiveRepresentativesandDistributors.Forcollaborationopportunitiespleasecontactusinfo@altechna.com

Balticstates&Belarus Balticstates Israel,BelarusLithuania


Andor TechnoLogyPRODuCTPORTFOLIO

Globalleaderinthedevelopmentandmanufactureofhighper-formance scientific digital cameras for academic, industrial and government applications.

Imagingcameras

eMccd

WiththeiXonEMCCDcameras,Andorhavedeliveredadedicat-ed, truly high-end, yet accessible ultrasensitive scientific camera platform, designed specifically to drive the absolute best from EMCCDtechnologyacrossallcriticalperformancespecsandpa-rameters

scMoS

unlike any CCD or CMOS camera to come before, Andor ’s 5.5megapixel sCMOS cameras are unique in their ability to com-bineultra-lownoise,extremelyrapidframerates,widedynamicrange,largefieldofviewandhigh-resolution.TheAndorsCMOSportfolio ensures a viable technical and commercial solution to allresearchandOEMapplicationanddesignrequiremnents.

iccd

Andor’siStar ICCDcameraseriesextracttheverybestfromCCDsensor and gated image intensifier technologies, achieving a superior combination of rapid acquisitions rates and ultra-high Sensitivitydowntosinglephoton.Exceptionaldetectionperfor-mances are accessed through high Quantum-Efficiency Imageintensifiers, Thermo-Electric cooling to -40°C, 500 kHz photo-cathodegatingratesandenhanced intensifierEBInoise reduc-tion.

Spectroscopy cameras

Market leading CCDs, InGaAs PDAs, Intensified CCDs and Elec-tron-MultiplyingCCDsforvuvtonIRSpectroscopy. unsurpassed combination of cutting edgeTher-mo-Electriccooling,proprietaryvacuumtechnology and ultra-low-noise electronics to extract the verybest performance from every Andor camera.

Spectrographs

Complete family of rugged, pre-aligned and precalibrated Cz-erny-Turner&Mechellespectrographs,forapplicationsrangingfromhigh-resolutionuvplasmastudiestonIR photoluminescence.The ideal partner for Andor ’s high-performance detectors and accessories for ultimate low-light detection.

Scanning Accessories

Extending Spectroscopy fromuv into Short and Long-Wave IRthrough a range of single point detectors including a PMTs, Siphotodiode, InGaAs, PbS, InSb and MCT. Software controlleddata acquisition unit synchronizes simultaneously detectors, monochromators and motorized accessories.

Accessories

From gratings to fibre optics, sample chamber, filter wheel and microscope coupling interfaces, each accessory allows seamless optimization of Andor detection system performance and easy integrationintoresearcherscomplexexperimentalsetups.


AeroTechPRODuCTPORTFOLIO

Stages

Aerotech manufactures a large selection of linear, rotary, lift, and Z-axispositioningstagesthatutilizeourownbrushlesslineardi-rect-drive servomotors, as well as ball-screw models driven with Aerotechbrushorbrushlessrotarymotors.Travelsforourlineartables range from 25mm to 1.5meters.Aerotech’s positioningstages are utilized in high-performance applications in indus-trial robots, fiberoptics and photonics, vision systems, machine tools, assembly, semiconductor equipment, medical component laser machining, micromachining, electronic manufacturing, and other industrial automation applications. Aerotech even offer a complete line of nanopositioning stages that provide nanometer resolution, accuracy, repeatability, and in-position stabilitywithtravelsfrom25mmto160mm.Inaddition,Aero-tech manufactures drives and motion controllers that perfectly complement our positioning stages.

Motioncontrollersanddrives

Aerotech motion controllers are used in positioning systems throughout theworld.TheAutomation3200multi-axismotioncontrollerissoftware-based(noPCslotsrequired)andmarriesarobust,highperformancemotionenginewithvision,PLC,robot-icsandI/Oinoneunifiedprogrammingenvironment.TheA3200

utilizes the industry standard FireWire® network to provide from 1to32axesofsynchronizedcontrolwithnodegradationinper-formanceastheaxiscountincreases.Aerotech manufactures drives for a wide range of industrial automation applications. Their drives power servomotors andcomplement Aerotech motion controllers in applications as di-verse as industrial robots, vision systems, assembly machines, machine tools, semiconductor manufacturing equipment, elec-tronic manufacturing and in a variety of other industrial control solutions.

Software

Aerotech offers a variety of integrated automation software solutions that are designed for quick, easy set-up, fast devel-opment and commissioning and unparalleled performance for bothsimpleapplicationsandthepoweruser.Withover40yearsofmotioncontrolexperience,they’relistenedtocustomersanddeveloped software that is flexible, scalable and provides theuser with the high-performance features they want and need, while simplifying and speeding the development of your appli-cationthroughintuitiveanduser-friendlyfeatures.Forexample,Motion Composer suite offers a Configuration Manager to or-ganize your applications, calculators for quick and easy setup, extensive diagnostics to speed commissioning, an IntegratedDevelopment Environment for fast development, data acqui-sition and analysis tools to increase performance, all in a fully compliant.nET2.0environmentthatshortensthedevelopmentcycle. Add to that a complete line of complementary software tools available for eachof our controller platforms (A3200, En-sembleandSoloist),andyouhaveatrulyrobust,intuitive,high-performance software platform in which to develop your unique application.


SeMrockPRODuCTPORTFOLIOSemrock offer a wide range of hard-coated filter products and accessories that support the life science, laser and optical sys-tem market. They manufacture optical filters for fluorescencemicroscopy, Raman spectroscopy, and laser systems aswell asour own filter holders.

SemrockFiltersDon’tBurnOut

AllSemrockfiltersarehardcoatedwithsophisticatedIonBeamSputtering (IBS) technology, resulting inpatentedstate-of-the-artfilterswithextremelydurablehardglasscoatingsonasinglehard glass substrate. no absorbing glass and no lamination isnecessary.Theresultisexceptionallydurable“noburnout”fluo-rescence filters of the highest performance.

Semrock Filters Optimized forMultiphotonMicroscopy

Semrock has brought enhanced performance to multiphoton users by introducing optical filters with ultra-high transmission, verysteepedgesandcarefullyoptimizedblocking. Givenhowmuch investment is typically required for the excitation laserand other complex elements ofmultiphoton imaging systems,thesenewfiltersrepresentasimpleandinexpensiveupgradetosubstantially boost system performance.The BrightLine® emission filters provide crystal-clear transmis-sion from the near-uv to the near-IR and provide deep block-ingacrosstheTi:Sapphirelasertuningrange,whichiscriticaltoachieving high signal-to-noise ratio and measurement sensitiv-ity.

Optical Filters for Laser-basedFluorescenceMicroscopes

Dichroics designedfor laser fluorescence applications are coat-ed with an antireflec-tive coating in order tomaximizetransmis-

sion of the emission signal and eliminate coherent interference artifacts. A powerful laser excitationbeam can encourage au-tofluorescence that will contaminate the emission signal, so a substrate with very low autofluorescence, such as fused silica, should be used.Thedichroicbeamsplittercanhavea significant impacton theimage quality in certain applications, especially if the flatness (orcurvature)ofthedichroicsisnotsuitable.Formostlaserfluo-rescence applications, the dichroic should be flat enough that there is no noticeable focal shift, where focal shift is typically defined by the Rayleigh range. This is critical for applicationssuchasTIRFmicroscopyandstructuredillumination.

TunableBandpassFilters

Fluorescence microscopy applications, hyperspectral imaging, high-throughput spectroscopy, and fiber-optic telecommunica-tionssystemscanallbenefit fromtunableoptical filters. Thereexist several technologies that combine the two-dimensionalimaging performance characteristics of thin-film filters and the centerwavelength tuning flexibilityofadiffractiongrating, in-cluding liquid-crystal tunable filters, acousto-optic tunable fil-ters, and linear-variable filters, but none are ideal and all have significant additional limitations.BecauseofthatSemrockhasdevelopedarevolutionarynewop-tical filter technology: Thin-film filters that are tunable over awide range of wavelengths by adjusting the angle of incidence.

ultraviolet(uv )RamanSpectroscopy

As an increasing number of compact, affordable, and high-power uv lasers have become available, like the quadrupled,diode-pumped nd:yAG lasers at 266 nm and neCu hollow-cathodemetal-ion lasersat248.6nm,ultra-sensitiveuvRamanspectroscopy has become a more common technique. Optical filteravailabilityintheuvrange,however,hascontinuedtolagbehind.Semrockisproudtoofferanumberofextremelyhigh-performance filters that are ideal for uv Raman spectroscopy.RazorEdge®long-wave-passfiltersandMaxLine®laser-linefiltersofferaselectiontocomplementthemostpopularuvlasers.


oceAn opTicSPRODuCTPORTFOLIOSpectrometers

OceanOpticsoffersnext-generationscientific-gradespectrom-eters with high sensitivity and low stray light performance that make it ideal for a wide range of low light level applications such asfluorescence,DnAsequencingandRamananalysis.

They have an athermal design that promotes excellent spec-trometer wavelength stability, triggering functions for providing accurate timing and synchronization between the spectrometer and other devices and a replaceable slit design for added con-venience.Anextensiverangeofgratingsoffersflexibilityinop-timizing applications.

Light sources

Ocean Optics light sources for illumination cover various wave-length ranges to enable absorbance, transmission and reflec-tancemeasurementsfromthedeepuvtothemid-infrared.Light-emitting diodes produce output for fluorescence mea-surements. For fast, reliable spectrometer wavelength calibra-tions, they also offer a range of options.

Optical Fiber Assemblies

Ocean Optics Premium-grade Optical Fiber Assemblies consis-tentlydeliveruniformresultswithminimalsignalvariance.Pre-mium-gradeAssemblies includehigh-qualitySMA905connec-torsandsilicone-coatedsteelmonocoiljacketingwithanomexbraidforsuperiorstrainrelief.EachPremium-gradeAssemblyisshippedwithaQAreport that includesboth theserialnumberand transmission curve of the assembly

Metrology

Ocean Optics offers range of high-precision metrology tools for thin film measurement, plasma analysis and optical character-ization are fully integrated with software and applications da-tabasesupport.Eachofthesemetrologyproducts incorporatesOcean Optics miniature fiber optic spectroscopy technology.

Software

Ocean Optics offers a comprehensive library of data acquisition and display software products for a variety of spectroscopic ap-plications. SpectraSuite is a modular, Java-based spectroscopy software platform that operates on Windows, Macintosh andLinux operating systems, and includes modules for irradianceand color measurement. SpectraSuite is the software platform on which all Ocean Optics software will be built. In addition to the products listed here,custom software development services are available.


GTIchirpedmirror• Reflectivityupto99,9%.• Centralwavelengthtoleranceupto1%.

• GDDvaluesrangesfrom100to1500fs2foryb:KGW,yb:yAGlaser type coatings according to customer specifications.

• CalculatedandmeasuredGDDcurves are supplied with every batch.

yb:CaF2LasercrystalDuetoyb:CaF2crystallowquantumdefect and a comparably long fluorescence lifetime, ytterbium-doped gain media are preferably utilized for high-power diode-pumped systems and laser amplifiers with high optical-to-optical conversion efficiencies.

nd:yLFLasercrystal• Lowinhomogeneity• Aperturesupto20mm• Lengthupto120mm• Barrelsidecanbeoptimizedfor

better heat handeling

Large apertureWattPilotattenuator• Polarizers:120x40mm,thicknessvariesfrom4to12mm.

• Air-spacedwaveplatewithCA=Ø40mm.

• Totalweight:1.1kg.

nEWPRODuCTSAnDnEWS

IRviewer• Highperformance• Compact(0.28–0.42kg)• Lowcost(startingfrom890EuR)• Widespectralrange(from350nmto2000nm)

Achromatic waveplates• Zeroorderwavepalteswithanairspace;

• Retardanceoverentirecoatingrage:450–650nm,650–1100nm,900–2100nm;

• Retardationtolerancebetterthanλ/100;

• BroadbandARcoatings.

Laser optics directlyfrom stockAltechna e-shop ‘In Stock Op-tics’ offers a wide range of laseroptics directly from stock. visitwww.instockoptics.com and order onlinefromourextensivestockofop-tical components which are listed live and available at real time. We assure worldwide dispatch within 1 week.

ISO9001Altechnais certified with the ISO9001 quality management systemcertification confirming that the company sells lasers, optic components and related products and services complying with the ISO9001standardrequirements.


TOPPRODuCTS

Axicons• Planoconvex,planoconcaveanddoubleconvexavailable;

• Producesringshapedimageinthefarfield;

• Availablediameterupto50mm;• variousARcoatingsareavailable;• Customdesignproductionis

available.

PolarizingCubesforHighPowerApplications• Opticallycontacted;• Damagethreshold>20J/cm2at1064nm10ns;

• Extinctionratiobetterthan35dB.

Broadband(ultrafast)ThinFilmPolarizers• Efficientlyseparatesthes-andp-polarizationcomponents;

• Optimisedforpopularlaserwavelengths;

• Manybroadband(ultrafast)thinfilm polarizers are available in stock.

Mid-IRwaveplates• ZOwaveplatesformid-IRapplications(2.8-9.0microns);

• Customsizeavailable;• Customdesignwaveplatesare

available in small and mass production quantities.

yb:KGW,yb:KyW,yb:yLF,yb:CaF2lasercrystals• Highabsorptioncoefficient@980nm;

• Highstimulatedemissioncrosssection;

• Lowlasingthreshold;• Extremelylowquantumdefect;• Broadoutputat1020-1060nm;• Highslopeefficiencywithdiodepumping(>55%);

• Highyb-dopingconcentration.

Ti:Sapphirecrystals• Broadlasingrange:660-1050nmband;

• Perfectforultrashortpulsegeneration;

• Highgainandhighpowerlasing;• Highopticalqualityandbulkdamagethreshold;

• Customdesignproductionisalsoavailable;

• Differentdopinglevelsavailable.

MotorizedlaserbeamattenuatorWattPilot• user-friendlysoftwareinterface;• Highrotationstepresolution(0,4mrad/step);

• negligiblebeamdeviation;• Stand-aloneuSBpoweredcontroller;

• Easytointegrate.


ORDERInGInFORMATIOn:

Ordersmaybeplacedbymail,e-mailor fax.Mailordersshouldbe sent to:

techna

LT-08 Vilnius, LiThUAniA

For prompt orders please send the purchase order number via e-mail [email protected] or fax +370 5 272 3704.

For your convenience you may order products directly from our representative in your country.

OnLInESHOPPInG

Topurchaseitemsonline,simplyfollowthestepslistedbelow:

1. Find an item by browsing the product menu or by entering theproductname in the“Search”window. Ifyoucannot findtheproduct intheStocklistandamongtheCatalogue items,youarewelcometofillintheRequestformwithyourdesiredcustom parameters.

2. Once your find the product you want to purchase, click .3. Ifyouwanttobuymoreitems,click“Continueshopping”and

repeat the first two steps.4.When you finish selecting the products, click“My Basket” at

the top corner of the website.

5. If you choose one or more Custom items (the price is notdefined on the website) you can send the Request directlyto the sales engineer who will contact you within 24 hourswith theQuotation. Ifallofyour itemsare fromtheStocklistor from theCatalogue you canplace your order directly byclicking“Continue”.Thenfollowthesesteps:

5.1. Fill in billing information. If the billing information is the same as the shipping

information, check the box ”Ship to this address” andpress“Continue”.

If the billing information is different from the shippinginformation, select “new Address” from the dropdownmenu,fillintheshippinginformationandpress“Continue”.

5.2. Select delivery type. Ifyouchoose“Deliveryunderyourcarrieraccount”,select

the carrier, type your account number with carrier and press“Continue”.

If you select “Delivery organized by Altechna”, you willbe charged for the freight costs. For next step press“Continue”.

5.3.Checkthebillingandshippinginformation.Ifitneedsanychanges,press“Back”;otherwise,press“Continue”.

5.4.Selectpaymentmethodandpress“Continue”. If you select payment by Paypal, you will be redirected

to Paypal account. For further operations followPaypal’sinstructions.

If you choose bank transfer, follow transfer information.youmayalsoselect“Purchaseorder”andenteritsnumberfor further reference.

5.5.Forfurthershoppingpress“Backtoshop”.

Learn more with online shop demo video:


PAyMEnTTERMS

Paymentscanbemadeby30netdaysby:

A. payment by bank transfer.Directfundsto: IBAn:LT087044060001103426withABSEB Bankcode70440,Gediminoave.12, LT-01103vilnius,Lithuania,SWIFT:CBvILT2X

B. payment by cheque. Address cheque to: UAB ALTECHnA,Mokslininku st.6A, LT-08412 vilnius,

Lithuania

c. payment with credit cards (Mastercard, ViSA):1.Inordertomakeapaymentviacreditcard,youhavetobe

registeredinourwebsite.Ittakesjustcoupleofminutes.2. Once logged onto our website you have to enter “Pay

Online”.3.Pleasefollowon-screeninstructionsforpayingonline(you

willberedirectedtoPayPal).4.Additional3%chargemaybeapplied.

Advance payment is requested for the first order only.

WARRAnTy

Allproductsareguaranteedtobefree fromdefects.Claimsareaccepted for a period of three months after delivery. We do not assume liability for installation, labor or consequential damages.

InSTOCKOPTICS-LASEROPTICSDIRECTLyFROMSTOCK

Altechna e-shop ‘In Stock Optics’ offers a wide range of laseroptics directly from stock. visit www.instockoptics.com andorder online from our extensive stock of optical componentswhich are listed live and available at real time. We assure worldwide dispatch within 1 week.

Ourextensiverangeoflaseropticsincludes:

• uncoatedLaserOptics(Lenses,Prisms,Windows,Filters)• Coated Laser Optics (Mirrors, Wavelength Separators, ARCoatedwindows,Filters)

• Polarization Optics (Waveplates, Polarizing Cubes, BrewsterTypeThinFilmPolarizers,Glanandotherpolarizers)

• Laser&nonlinearCrystals( Ti:Sapphire,nd:yvO4,BBO,KDPandotherCrystals)

All products are inspected in Altechna metrology laboratory and fitsISO9001:2008qualitystandards.

For more information please visit www.instockoptics.comor contact [email protected]

FemtoSolutions.eu-yOuREXPERTInuLTRAFASTOPTICS

FemtoSolutions is an e-shop dedicated only to products related to ultrashort pulse phenomena. Best solutions for the mostdemanding femtosecond systems are available just in one place.

visit www.femtosolutions.eu and select from morethan1000highqualityproductsfrom:

1. Femtosecond components2. Femtosecond accessories3. Femtosecond sources4.Femtosecondmicromachiningsystems

For more information please visit www.instockoptics.comor contact [email protected]



TABLEOFCOnTEnTS:About us 2

Partnersanddistributors 4

Representedcompanies 5

newproductsandnews 10

Topproducts 11

Ordering information 12

1.GEnERALOPTICS 17

unCOATEDOPTICALWInDOWS/SuBSTRATES 18

LEnSES 20

Plano-Convexlenses 20

Plano-Concavelenses 23

Double-Convexlenses 26

Double-Concavelenses 28

PositiveCylindricallenses 30

negativeCylindricallenses 32

Meniscuslenses 34

Achromatic lenses 36

LensCase 38

AXICOnS(COnICALLEnS) 40

Plano-Convexaxicons 40

Plano-Concaveaxicons 42

Double-Convexaxicons 44

PRISMS 46

Dispersingprisms 46

Right-Angleprisms 48

Right-Angleprism-retroreflectors 50

CornerCuberetroreflectors 51

DIELECTRICCOATEDOPTICS 52

HRlaserlinemirrors(HR) 52

HRbroadbandmirrors(BBHR) 54

Partialreflectingmirrors(PR) 56

GTIchirpedmirror 58

Wavelength separators 60

Duallaserlinemirrors(DHR) 62

ARcoatedwindows(AR) 64

BroadbandARcoatedwindows(BBAR) 66

DualARcoatedwindows(DAR) 68

METALLICCOATEDOPTICS 70

FILTERS 72

Colorglassfilters 72

Interferencefilters 75

neutraldensityabsorptiontypefilters 77

Circularvariableneutraldensityfilters 79

METALMIRRORS 81

vARIABLEREFLECTIvITyMIRRORS 83

nOnPOLARIZInGBEAMSPLITTERCuBES 84

COATInGSSECTIOn 86

DIELECTRICCOATInGS 86

HRlaserlinecoatings(HR) 87

HRbroadbandcoatings(BBHR) 89

Partialreflectingcoatings(PR) 90

Wavelength separating coatings 92

Duallaserlinecoatings(DHR) 94

LaserlineARcoatings(AR) 95

BroadbandARcoatings(BBAR) 96

DualARcoatings(DAR) 97

METALLICCOATInGS 98

2.POLARIZATIOnOPTICS 99

WAvEPLATES(PHASERETARDATIOnPLATES) 100

Crystallinequartzwaveplates 101

Highpowerwaveplates 103

Achromatic(broadband)waveplates 105

Mid-IRwaveplates 107

SPECIALOPTICSS-WAvEPLATE 108

BREWSTERTyPETHInFILMPOLARIZERS 109

BROADBAnD(uLTRAFAST)THInFILMPOLARIZERS 111

POLARIZInGCuBES 113

GLAnAnDOTHERTyPEPOLARIZERS 115

HighpowerlaserGlanpolarizers 115

GlanTaylorpolarizers 117

GlanThompsonpolarizers 119

Wollaston polarizers 120

Beamdisplacers 122

Rochonpolarizers 123

3.LASERAnDPASSIvEQ-SWITCHCRySTALS 125

LASERCRySTALS 126

Ti:Sapphirecrystals 126

nd:yvO4 crystals 128

nd:yAGcrystals 130

nd:yLFcrystals 132

nd:KGWcrystals 133

yb:KGWandyb:KyWcrystals 135

yb:CaF2crystals 139

yb:yAGcrystals 139

PASSIvEQ-SWITCHCRySTALS 140

Cr4+:yAGcrystals 140

v3+:yAGcrystals 142

Co:Spinelcrystals 144

4.nOnLInEAROPTICS 146

nOnLInEARCRySTALS 147

BBOcrystals 147

LBOcsrytals 147


KTPcrystals 151

KDP,DKDPcrystals 153

LinbO3 crystals 155

AgGaSe2 crystals 156

AgGaS2 crystals 156

ZnGeP2 crystals 157

PHOTOREFRACTIvECRySTALS 158

SBncrystals 158

BSOcrystals 160

Fe:LinbO3 crystals 162

RAMAnCRySTALS 164

5.LASERSAnDLASERSySTEMS 165

CWLASERS 166

DLCWbluevioletlaser,405nm 166

DPSSCWbluelaser,457nm 167

DPSSCWbluelaser,473nm 168

DPSSCWgreenlaser532nm 169

DPSSCWyellowlaser593.5nm 170

DPSSCWredlaser671nm 171

DPSSCWIRlaser1064nm 172

DLCWIRlaser1550nm 173

TInyDIODELASER 174

EDuCATIOnALDPSSLASERKIT 175

6. LASERACCESSORIESAnDEQuIPMENT 176

WATTPILOT 177

StandardWattPilot 177

EnhancedWattPilot 179

ultrafastWattPilot 181

MotorizedWattPilot 183

LASERACCESSORIESAnDEQuIPMEnT 186

Beamexpanders 186

Motex-motorizedtunablebeamexpander 188

Laser beam shaping systems 189

Autocorrelators 192

Highpowerlasershutters 196

Beamdumps 197

IRviewer 198

Laser visualizers 199

Spectacles and goggle type safety glasses 200

Laser diodes and modules 203

Optical chopper 204

7.OPTOMECHAnICS 205

OPTICALTABLES 206

BASEMOunTSAnDACCESSORIES 207

Postmountings 207

Adapters 208

Postcollars,clampsandbaseplates 208

OPTICALMOunTSAnDHOLDERS 211

Optical mounts 211

Optical holders 213

OPTICALPOSITIOnERS 215

Stainless steel kinematic mounts 215

Repositioningmounts 217

Polarizerholders 218

Twoaxistiltmounts 220

Precisionopticalmountsofsidecontrol 222

Two/threeaxistilt/translationmounts 223

Mirrormounts/tiltplatformsofsidedrive 226

Special positioners 229

Budgetkinematicopticalmounts 231

BASEPOSITIOnERS 232

TRAnSLATIOnAnDROTATIOnSTAGES 234

Rotationstages 234

narrowtranslationstages 236

Lowprofiletranslationstages 237

Microtranslationstages 239

verticalpositioners 239

Dovetaillineartranslationstages 240

MOTORIZEDPOSITIOnERSAnDCOnTROLLERS 241

Translationstages 241

Rotationstages 244

verticaltranslationstages 248

MOTORIZEDATTEnuATORS 254

8.SERvICES&OPTICALMATERIALS 255

METROLOGyTESTS 256

MEASuREMEnTSETuPS 258

LASERAnDnOnLInEARCRySTALREPOLISHInGSERvICES 261

OPTICALMATERIALS 262

9. WORKSHOPOFPHOTOnICS 263

COMPAnyPROFILE 264

FEASIBILITySTuDyOnLASERMICROMACHInInG 264

LASERPROCESSDEvELOPMEnT 265

SMALLSCALEPRODuCTIOn 265

CuSTOMLASERSySTEMSFORLABORATORy 266

FemtoLAB 266

SOLLAS 267

nSCuLPTOR 267

DEvELOPMEnTOFInDuSTRIALLASERMACHInES 268

FemtoFAB 268

SOFTWAREFORLASERMICROMACHInInG 269

FEMTOSECOnDLASERMACHInInG 270

Samples of femtosecond micromachining technology 271

MuLTIPHOTOnPOLyMERIZATIOnTECHnOLOGy 279

MPPapplications 281

ILLuSTRATIOnSSOuRCE 283


GEnERALOPTICS

unCOATEDOPTICALWInDOWS/ SuBSTRATES

18

LEnSES 20

•Plano-Convexlenses 20

•Plano-Concavelenses 23

•Double-Convexlenses 26

•Double-Concavelenses 28

•PositiveCylindricallenses 30

•negativeCylindricallenses 32

•Meniscuslenses 34

•Achromatic lenses 36

•LensCase 38

AXICOnS(COnICALLEnS) 40

•Plano-Convexaxicons 40

•Plano-Concaveaxicons 42

•Double-Convexaxicons 44

PRISMS 46

•Dispersingprisms 46

•Right-Angleprisms 48

•Right-Angleprism-retroreflectors 50

•CornerCuberetroreflectors 51

DIELECTRICCOATEDOPTICS 52

•HRLaserLinemirrors(HR) 52

•HRBroadBandmirrors(BBHR) 54

•Partialreflectingmirrors(PR) 56

•GTIchirpedmirror 58

•Wavelength separators 60

•DualLaserLinemirrors(DHR) 62

•ARcoatedwindows(AR) 64

•BroadBandARcoatedwindows(BBAR) 66

•DualARcoatedwindows(DAR) 68

METALLICCOATEDOPTICS 70

FILTERS 72

•Colorglassfilters 72

• Interferencefilters 75

•neutralDensityAbsorptionTypefilters 77

•CircularvariableneutralDensityfilters 79

METALMIRRORS 81

vARIABLEREFLECTIvITyMIRRORS 83

nOnPOLARIZInGBEAMSPLITTERCuBES 84

COATInGSSECTIOn 86

DIELECTRICCOATInGS 86

•HRLaserLinecoatings(HR) 87

•HRBroadBandcoatings(BBHR) 89

•Partialreflectingcoatings(PR) 90

•Wavelength separating coatings 92

•DualLaserLinecoatings(DHR) 94

•LaserlineARcoatings(AR) 95

•BroadBandARcoatings(BBAR) 96

•DualARcoatings(DAR) 97

METALLICCOATInGS 98

/ www.altechna.com18

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Material BK7,uvFS,IRFS,CaF2,ZnSe,Sapphire,MgF

2.

Shape Round,rectangular

Surface quality 20-10Scratch&Dig(BK7,uvFS);40-20Scratch&Dig(ZnSe,Sapphire,CaF

2,

MgF2)

Surfacefigureλ/10-λ/8per1inchdiam(BK7,uvFS)λ/2-λ/4per1inchdiam(ZnSe,Sapphire,CaF

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MgF2)

DimensiontolerancesDiameter:+0.0/-0.1mmThickness:±0.1mm

Coatings none.PleaserefertotheCoatingsSection

unCOATEDOPTICALWInDOWS/SuBSTRATES

variousdimensionssubstratesmadefromBK7,uvFS,IRFS,CaF2,ZnSe,Sapphire,MgF2.

Standard substrates are laser grade polished on both surfaces. These substrates are ideal for beamsplitters, windows, partialreflecting mirrors etc.

Laser components require highly polished substrates as well as high performance coatings. Scattering, damage of laser light can occur if the substrate is made of inferior material or if it is inadequately polished. For uv, very high power applicationsand ultrashort pulses we recommend using uvFS substrates.BK7 substrates are economical solution for laser componentsused in many applications in laboratory as well as in devices and instruments.

ALTECHnA provides various dielectric and metallic coatings on optical substrates.

Description

Standard specifications

Features

Miscellaneous

• Idealforbeamsplitters,windows,partialreflectingmirrorsetc• uvFSsubstratesarerecommendedfortheuvandveryhigh

energy applications• Windowsupto500mmdiameterareavailable

• Customdesignproductionisavailable• variousdielectriccoatingscanbedepositedonthese

substrates• Checkthestocklistitemsforfastestdelivery• Massproductioncapabilities:10’000piecespermonth

www.altechna.com / 19Ge

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• Beamsplitter / mirror mounts 5BM131 and5BM141(page220)

• 4OCM-opticalcomponentmounts(page212)

• 5OM37 - two angular fine adjustmentmounts(page223)

• Opticalcoatings(pages86-98)

MaterialDimensions,

mmParallelismError ProductID

Price*1-9pcs

BK7

12.7x3 <1arcmin 1-OS-1-0127-3 14€

12.5x5 <1arcmin 1-OS-1-0125-5 14€

12.7x6 <1arcmin 1-OS-1-0127-6 14€20x40x3 <20arcsec 1-OS-1-2040-3 34€

25.4x3 <1arcmin 1-OS-1-0254-3 18€

25.4x5 1˚±5arcmin 1-OS-1-1254-5 34€25.4x5 3˚±5arcmin 1-OS-1-3254-5 34€25.4x6 <1arcmin 1-OS-1-0254-6 18€30x6 <1arcmin 1-OS-1-0300-6 28€38.1x5 <1arcmin 1-OS-1-0381-5 28€50.8x8 <1arcmin 1-OS-1-0508-8 40€76.2x8 <1arcmin 1-OS-1-0762-8 48€

uvFS

12.7x2 <1arcmin 1-OS-2-0127-2 18€12.7x3 <1arcmin 1-OS-2-0127-3 18€12.7x5 <1arcmin 1-OS-2-0127-5 18€12.7x5 30arcmin±5arcmin 1-OS-2-1127-5 24€12.7x6 <1arcmin 1-OS-2-0127-6 18€20x40x3 <20arcsec 1-OS-2-2040-3 40€20x40x5 <20arcsec 1-OS-2-2040-5 40€20x60x5 1˚±5arcmin 1-OS-2-2060-5 50€20x60x2 <20arcsec 1-OS-2-2060-2 50€25.4x3 <1arcmin 1-OS-2-0254-3 22€25.4x5 <1arcmin 1-OS-2-0254-5 22€25.4x3 1˚±5arcmin 1-OS-2-1254-3 40€25.4x3 3˚±5arcmin 1-OS-2-3254-3 40€30x5 <1arcmin 1-OS-2-0300-5 40€

30x30x5 <1arcmin 1-OS-2-3030-5 40€38.1x5 <1arcmin 1-OS-2-0381-5 40€50.8x6 <1arcmin 1-OS-2-0508-6 60€76.2x6 <1arcmin 1-OS-2-0762-6 80€

IRFS12.7x6 <1arcmin 1-OS-3-0127-6 28€25.4x3 <1arcmin 1-OS-3-0254-3 36€

ZnSe 25.4x3 <1arcmin 1-OS-4-0254-3 60€CaF

225.4x3 <1arcmin 1-OS-5-0254-3 50€

MgF2

25.4x3 <1arcmin 1-OS-6-0254-3 50€Sapphire 25.4x3 <1arcmin 1-OS-7-0254-3 40€

CatalogItems

*[email protected]

Ifyoudonotfindsuitablesizeorneed other wavelengths design for your application please contact us and we guaranty to provide a solution for you

Relatedproductsandaccessories


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Material BK7,FS,uvFS,CaF2,ZnSe,Si,Ge

Diametertolerance +0.00/-0.15mm

Focal length tolerance ±3%

Centration <3 arcmin

Clearaperture >90%

Chamfer 0.25mm@45°

Surfacefigure λ/[email protected]

Surface quality 40-20Scratch&Dig

Designwavelength 632.8nm

ARcoatings none.PleaserefertotheCoatingsSection

PLAnO-COnvEXLEnSES(PCX)

PCX positive focal length lenses have flat surface on one sideand spherical surface on the other.They are used for focusingbeams in telescopes, collimators or condenser systems, optical transceivers or other applications. ALTECHnAprovidesPCXlensupto500mmdiameter.undercustomersrequestlensareanti-reflectioncoated(PleaserefertotheCoatingsSection).

Description


Features

Miscellaneous

• Convergesincidentlight• Customfocallengthavailablefrom1.5mmupto25000mm• Customdiameteravailableupto500mm

• Customdesignproductionisalsoavailable• Massproductioncapabilities:10’000piecespermonth• variousdielectriccoatingscanbedepositedonlenses• Checkonlinestockforattractivepricesandfastestdelivery


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Diameter,mm

Focal length, mm

Edgethickness, mm

ProductIDPrice

*l-9pcs

12.7

+20 2.5 1-PCX-1-A127 22€+25 2.5 1-PCX-1-B127 22€+40 2.5 1-PCX-1-C127 18€+50 2.5 1-PCX-1-D127 18€+60 2.5 1-PCX-1-E127 18€+75 2.5 1-PCX-1-F127 18€+100 2.5 1-PCX-1-G127 18€+150 2.5 1-PCX-1-H127 18€+200 2.0 1-PCX-1-J127 18€+250 2.0 1-PCX-1-K127 18€+300 2.0 1-PCX-1-L127 18€+500 2.0 1-PCX-1-M127 18€+1000 2.0 1-PCX-1-n127 18€+1500 2.0 1-PCX-1-P127 18€

25.4

+35 2.0 1-PCX-1-A254 26€+50 2.0 1-PCX-1-B254 20€+60 2.0 1-PCX-1-C254 20€+75 2.0 1-PCX-1-D254 20€+100 2.0 1-PCX-1-E254 20€+125 2.0 1-PCX-1-F254 20€+150 2.0 1-PCX-1-G254 20€+200 2.0 1-PCX-1-H254 20€+250 2.0 1-PCX-1-J254 20€+300 2.0 1-PCX-1-K254 20€+400 2.0 1-PCX-1-L254 20€+500 2.0 1-PCX-1-M254 20€+750 2.0 1-PCX-1-n254 20€+1000 2.5 1-PCX-1-P254 20€+1200 2.5 1-PCX-1-R254 20€+1500 2.5 1-PCX-1-S254 20€+2000 3.0 1-PCX-1-T254 22€+2500 3.0 1-PCX-1-u254 22€+3000 3.0 1-PCX-1-v254 22€+4000 3.0 1-PCX-1-W254 22€+5000 3.0 1-PCX-1-X254 22€+10000 3.0 1-PCX-1-y254 26€

50.8

+200 3.0 1-PCX-1-A508 48€+300 3.0 1-PCX-1-B508 48€+350 3.0 1-PCX-1-C508 48€+500 3.0 1-PCX-1-D508 48€+1000 3.0 1-PCX-1-E508 48€+2000 3.0 1-PCX-1-F508 48€

CatalogItems

Diameter,mm

Focal length, mm

Edgethickness, mm

ProductIDPrice

*l-9pcs

12.7

+20 2.5 1-PCX-2-A127 38€+25 2.5 1-PCX-2-B127 36€+40 2.5 1-PCX-2-C127 36€+50 2.5 1-PCX-2-D127 32€+60 2.5 1-PCX-2-E127 32€+75 2.5 1-PCX-2-F127 32€+100 2.5 1-PCX-2-G127 32€+150 2.5 1-PCX-2-H127 32€+200 2.0 1-PCX-2-J127 32€+250 2.0 1-PCX-2-K127 32€+300 2.0 1-PCX-2-L127 32€+500 2.0 1-PCX-2-M127 32€+1000 2.0 1-PCX-2-n127 32€+1500 2.0 1-PCX-2-P127 32€

25.4

+35 2.0 1-PCX-2-A254 45€+50 2.0 1-PCX-2-B254 40€+60 2.0 1-PCX-2-C254 40€+75 2.0 1-PCX-2-D254 40€+100 2.0 1-PCX-2-E254 40€+125 2.0 1-PCX-2-F254 40€+150 2.0 1-PCX-2-G254 40€+200 2.0 1-PCX-2-H254 40€+250 2.0 1-PCX-2-J254 40€+300 2.0 1-PCX-2-K254 40€+400 2.0 1-PCX-2-L254 40€+500 2.0 1-PCX-2-M254 40€+750 2.0 1-PCX-2-n254 40€+1000 2.5 1-PCX-2-P254 40€+1200 2.5 1-PCX-2-R254 40€+1500 2.5 1-PCX-2-S254 40€+2000 3.0 1-PCX-2-T254 44€+2500 3.0 1-PCX-2-u254 44€+3000 3.0 1-PCX-2-v254 44€+4000 3.0 1-PCX-2-W254 44€+5000 3.0 1-PCX-2-X254 44€+10000 3.0 1-PCX-2-y254 48€

50.8

+200 3.0 1-PCX-2-A508 110€+300 3.0 1-PCX-2-B508 110€+350 3.0 1-PCX-2-C508 110€+500 3.0 1-PCX-2-D508 110€+1000 3.0 1-PCX-2-E508 110€+2000 3.0 1-PCX-2-F508 110€

Bk7 plano-convex Lenses UVFS plano-convex Lenses


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• 4SCML-2–sel f-center ing lens/opticsmount(page211)

• 5TLM-1–y-Zpositionerforlens,pinholesandobjec-tives(page230)

• Opticalcoatings(pages86-98)• Double-Convexlenses(page26)

• Achromaticlenses(page36)

RelatedproductsandaccessoriesMaterial

Diameter,mm

Focal length, mm

Edgethickness, mm

ProductIDPrice

*l-9pcs

CaF2

25.4 +100 3.0 1-PCX-3-A254 90€25.4 +200 3.0 1-PCX-3-B254 90€25.4 +500 3.0 1-PCX-3-C254 90€25.4 +1000 3.0 1-PCX-3-D254 90€

ZnSe

12.7 +25 3.0 1-PCX-4-A127 115€12.7 +30 3.0 1-PCX-4-B127 115€12.7 +50 2.5 1-PCX-4-C127 110€12.7 +100 2.5 1-PCX-4-D127 110€12.7 +200 2.5 1-PCX-4-E127 110€12.7 +300 2.5 1-PCX-4-F127 110€12.7 +500 2.5 1-PCX-4-G127 110€25.4 +100 2.5 1-PCX-4-A254 115€25.4 +200 2.5 1-PCX-4-B254 115€25.4 +300 2.5 1-PCX-4-C254 115€25.4 +500 2.5 1-PCX-4-D254 115€

plano-convex Lenses from other materials

*[email protected]


CatalogItems


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Clearaperture >90%

Chamfer 0.25mm@45°





PLAnO-COnCAvELEnSES(PCv)

PCvnegativefocallengthlenseshaveaflatsurfaceononesideand a spherical surface on the other.They are used to expandbeams or to increase focal lengths in optical systems or other similar applications. ALTECHnAprovides PCv lenses up to 500mm in diameter. Under customers request lenses are anti-reflectioncoated(PleaserefertotheCoatingsSection).

Description


Features

Miscellaneous

• Divergesincidentlight• Customfocallengthavailablefrom1.5mmupto25000mm• Customdiameteravailableupto500mm

• Customdesignproductionisalsoavailable• Massproductioncapabilities:10’000piecespermonth• variousdielectriccoatingscanbedepositedontheselenses• Checkonlinestockforattractivepricesandfastestdelivery


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Diameter,mm

Focal length, mm

Edgethickness, mm

ProductIDPrice

*l-9pcs

12.7 -20 4.0 1-PCv-1-A127 22€12.7 -30 3.5 1-PCv-1-B127 22€12.7 -50 3.5 1-PCv-1-C127 18€12.7 -75 3.5 1-PCv-1-D127 18€12.7 -100 3.5 1-PCv-1-E127 18€12.7 -150 3.5 1-PCv-1-F127 18€12.7 -200 3.5 1-PCv-1-G127 18€12.7 -250 3.5 1-PCv-1-H127 18€12.7 -500 3.5 1-PCv-1-J127 18€12.7 -1000 3.5 1-PCv-1-K127 18€25.4 -40 6.0 1-PCv-1-A254 20€25.4 -50 5.5 1-PCv-1-B254 20€25.4 -75 5.0 1-PCv-1-C254 20€25.4 -100 4.0 1-PCv-1-D254 20€25.4 -150 3.5 1-PCv-1-E254 20€25.4 -200 3.5 1-PCv-1-F254 20€25.4 -250 3.5 1-PCv-1-G254 20€25.4 -300 3.5 1-PCv-1-H254 20€25.4 -400 3.5 1-PCv-1-J254 20€25.4 -500 3.5 1-PCv-1-K254 20€25.4 -1000 3.5 1-PCv-1-L254 20€25.4 -2000 3.5 1-PCv-1-M254 22€25.4 -3000 3.5 1-PCv-1-n254 22€

25.4 -10000 3.5 1-PCv-1-P254 24€

50.8 -500 4.0 1-PCv-1-A508 48€50.8 -900 4.0 1-PCv-1-B508 48€50.8 -1000 4.0 1-PCv-1-C508 48€50.8 -1200 4.0 1-PCv-1-D508 48€50.8 -1500 4.0 1-PCv-1-E508 48€50.8 -2000 4.0 1-PCv-1-F508 48€50.8 -8000 4.0 1-PCv-1-G508 48€

Bk7 plano-concave Lenses

Diameter,mm

Focal length, mm

Edgethickness, mm

ProductIDPrice

*l-9pcs

12.7 -20 4.0 1-PCv-2-A127 38€12.7 -30 3.5 1-PCv-2-B127 38€12.7 -50 3.5 1-PCv-2-C127 32€12.7 -75 3.5 1-PCv-2-D127 32€12.7 -100 3.5 1-PCv-2-E127 32€12.7 -150 3.5 1-PCv-2-F127 32€12.7 -200 3.5 1-PCv-2-G127 32€12.7 -250 3.5 1-PCv-2-H127 32€12.7 -500 3.5 1-PCv-2-J127 32€12.7 -1000 3.5 1-PCv-2-K127 32€25.4 -40 6.0 1-PCv-2-A254 40€25.4 -50 5.5 1-PCv-2-B254 40€25.4 -75 5.0 1-PCv-2-C254 40€25.4 -100 4.0 1-PCv-2-D254 40€25.4 -150 3.5 1-PCv-2-E254 40€25.4 -200 3.5 1-PCv-2-F254 40€25.4 -250 3.5 1-PCv-2-G254 40€25.4 -300 3.5 1-PCv-2-H254 40€25.4 -400 3.5 1-PCv-2-J254 40€25.4 -500 3.5 1-PCv-2-K254 40€25.4 -1000 3.5 1-PCv-2-L254 40€

25.4 -2000 3.5 1-PCv-2-M254 42€

25.4 -3000 3.5 1-PCv-2-n254 42€25.4 -10000 3.5 1-PCv-2-P254 46€50.8 -500 4.0 1-PCv-2-A508 110€50.8 -900 4.0 1-PCv-2-B508 110€50.8 -1000 4.0 1-PCv-2-C508 110€50.8 -1200 4.0 1-PCv-2-D508 110€50.8 -1500 4.0 1-PCv-2-E508 110€50.8 -2000 4.0 1-PCv-2-F508 110€50.8 -8000 4.0 1-PCv-2-G508 110€

UVFS plano-concave Lenses

CatalogItems


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Material Diameter,mm Focal Length, mm EdgeThickness,mm ProductID Price*l-9pcs

CaF2

25.4 -100 3.0 1-PCv-3-A254 90€25.4 -200 3.0 1-PCv-3-B254 90€25.4 -500 3.0 1-PCv-3-C254 90€25.4 -1000 3.0 1-PCv-3-D254 90€

ZnSe

12.7 -50 3.0 1-PCv-4-A127 115€12.7 -100 3.0 1-PCv-4-B127 110€12.7 -500 2.5 1-PCv-4-C127 110€25.4 -50 3.5 1-PCv-4-A254 115€25.4 -100 3.0 1-PCv-4-B254 115€25.4 -200 2.5 1-PCv-4-C254 115€25.4 -300 2.5 1-PCv-4-D254 115€

plano-concave Lenses from other materials

•4LM13-Self-centeringLens/OpticsMount

•Opticalcoatings(pages86-98)

CatalogItems

*[email protected]


•5ZyP-2-B1–y-Zpositionerforlens,pinholesandobjectives(page231)

•Double-Concavelenses(page28)

•Achromaticlenses(page36)


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Clearaperture >90%

Chamfer 0.25mm@45°





DOuBLE-COnvEXLEnSES(DCX)

Double convex or Biconvex lenses are symmetrical thereforehave equal radii of curvature on both sides. Biconvex lensesare used as magnifiers, objectives, condensing systems. Since bothsurfacescontributetothepowerofbiconvex lenses, theyhaveshorterfocallengththanPCXlensesofequaldiameterandsurfaceradius.Lensescanbeanti-reflectioncoated(PleaserefertotheCoatingsSection).

Description


Features

Miscellaneous

•Convergesincidentlight•LowersphericalaberrationsthanforPlano-Convexlenses• Customfocallengthavailable• Customdiameteravailable

• Customdesignproductionisalsoavailable• Massproductioncapabilities:10’000piecespermonth• variousdielectriccoatingscanbedepositedontheselenses• Checkonlinestockforattractivepricesandfastestdelivery


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Material Diameter,mm Focal length, mm Edgethickness,mm ProductID Price*l-9pcs

BK7

12.7 +12 2.0 1-BCX-1-A127 28€12.7 +15 2.0 1-BCX-1-B127 28€12.7 +20 2.0 1-BCX-1-C127 28€25.4 +25 2.0 1-BCX-1-A254 32€25.4 +30 2.0 1-BCX-1-B254 32€25.4 +35 2.0 1-BCX-1-C254 32€25.4 +50 2.0 1-BCX-1-D254 30€

uvFS

12.7 +15 2.0 1-BCX-2-A127 48€12.7 +20 2.0 1-BCX-2-B127 48€12.7 +25 2.0 1-BCX-2-C127 48€25.4 +30 2.0 1-BCX-2-A254 58€25.4 +40 2.0 1-BCX-2-B254 58€25.4 +50 2.0 1-BCX-2-C254 58€

• 4LM13-40-self-centeringlens/opticsmount(page211)


CatalogItems

*[email protected]


• 4LM149-10-universaladjustablelens/opticsmount(page212)

• Plano-Convexlenses(page20)



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Clearaperture >90%

Chamfer 0.25mm@45°





DOuBLE-COnCAvELEnSES(DCv)

Doubleconcaveorbiconcavelensesaresymmetricalwithequalradiiofcurvatureonbothsides.Thebiconcave lensesareusedin optical systems in combination with other lenses. Theselenses also work as beamexpanders, optical character readers,viewers and projection systems. Lenses can be anti-reflection coated(PleaserefertotheCoatingsSection).

Description


Features

Miscellaneous

• Divergesincidentlight• LowersphericalaberrationsthanforPlano-Concavelenses• Other dimensions are available in small and mass production

quantities• Massproductioncapabilities:10’000piecespermonth

• Customdesignproductionisalsoavailable• variousdielectriccoatingscanbedepositedontheselenses


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• 4SCML-4–self-centeringlens/opticsmounts(page211)


Material Diameter,mm Focal length, mm Edgethickness,mm ProductID Price*l-9pcs

BK7

12.7 -12 5.0 1-BCv-1-A127 32€12.7 -15 5.0 1-BCv-1-B127 30€12.7 -20 4.5 1-BCv-1-C127 28€25.4 -25 8.0 1-BCv-1-A254 38€25.4 -30 8.0 1-BCv-1-B254 34€25.4 -35 7.0 1-BCv-1-C254 32€25.4 -50 7.0 1-BCv-1-D254 30€

uvFS

12.7 -15 5.0 1-BCv-2-A127 52€12.7 -20 5.0 1-BCv-2-B127 48€12.7 -25 4.5 1-BCv-2-C127 48€25.4 -30 8.0 1-BCv-2-A254 60€25.4 -40 8.0 1-BCv-2-B254 58€25.4 -50 7.0 1-BCv-2-C254 58€

CatalogItems


*[email protected]


• 4OCM-25-opticalcomponentmount(page212)

• Plano-Concavelenses(page23)



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Material BK7,FS,uvFS,CaF2,ZnSe

Dimensionstolerance +0.00/-0.15mm



Clearaperture >90%

Chamfer 0.25mm@45°





POSITIvECyLInDRICALLEnSES

Cylindrical lenses with positive focal length condense lightin one dimension only. They are used to focus light to a thinline for effective harmonic generation in nonlinear crystals, in laser scanners, spectroscopy, dye lasers, acousto-optics or other applications. They are also irreplaceable for circularization ofdiode laser outputs, energy collection for linear detectors or for coupling to a slit input.

Description


Features

Miscellaneous

• Rectangularandroundshapeareavailable• Focus light in one dimension only

• Roundshapecylindricallensesareavailable• Customdesignproductionisalsoavailable• Massproductioncapabilities:10’000piecespermonth• variousdielectriccoatingscanbedepositedontheselenses• Checkonlinestockforattractivepricesandfastestdelivery


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• 4PH132-universalplateholder(page214)

• 5OM37-20-twoangularfineadjustmentmounts(page223)


Material Size, mm Focal length, mm ProductID Price*l-9pcs

BK7

10x10

+50 1-PCL-1-A100 44€+100 1-PCL-1-B100 44€+175 1-PCL-1-C100 44€+200 1-PCL-1-D100 44€+500 1-PCL-1-E100 44€+1000 1-PCL-1-F100 44€

20x20

+50 1-PCL-1-A200 48€+100 1-PCL-1-B200 48€+175 1-PCL-1-C200 48€+200 1-PCL-1-D200 48€+500 1-PCL-1-E200 48€+1000 1-PCL-1-F200 48€+2000 1-PCL-1-G200 48€

30x30

+200 1-PCL-1-A300 54€+500 1-PCL-1-B300 54€+1000 1-PCL-1-C300 54€+3000 1-PCL-1-D300 54€

uvFS

10x10

+50 1-PCL-2-A100 62€+100 1-PCL-2-B100 62€+175 1-PCL-2-C100 62€+200 1-PCL-2-D100 62€+500 1-PCL-2-E100 62€+1000 1-PCL-2-F100 62€

20x20

+50 1-PCL-2-A200 68€+100 1-PCL-2-B200 68€+175 1-PCL-2-C200 68€+200 1-PCL-2-D200 68€+500 1-PCL-2-E200 68€+1000 1-PCL-2-F200 68€+2000 1-PCL-2-G200 68€

30x30

+200 1-PCL-2-A300 78€+500 1-PCL-2-B300 78€+1000 1-PCL-2-C300 78€+3000 1-PCL-2-D300 78€

CatalogItems

*[email protected]



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Dimensionstolerance +0.00/-0.15mm



Clearaperture >90%

Chamfer 0.25mm@45°





nEGATIvECyLInDRICALLEnSES

Cylindricallenseswithnegativefocallengthexpandlightinonedimension only.They are used in laser scanners, spectroscopy,dye lasers, acousto-optics, optical processors or other applications. They are also irreplaceable for circularization ofdiodelaseroutputs.Lensescanbeanti-reflectioncoated(PleaserefertotheCoatingsSection).

Description


Features

Miscellaneous

• Rectangularandroundshapeareavailable• Divergeslightinonedimensiononly

• Roundshapecylindricallensesareavailable• Customdesignproductionisalsoavailable• Massproductioncapabilities:10’000piecespermonth• variousdielectriccoatingscanbedepositedontheselenses• Checkonlinestockforattractivepricesandfastestdelivery


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•4PH132-universalplateholder(214)

•4H29–pushholder(page213)



Material Size, mm Focal length, mm ProductID Price*l-9pcs

BK7

10x10

-50 1-nCL-1-A100 44€-100 1-nCL-1-B100 44€-180 1-nCL-1-C100 44€-200 1-nCL-1-D100 44€-400 1-nCL-1-E100 44€-500 1-nCL-1-F100 44€-600 1-nCL-1-G100 44€-1000 1-nCL-1-H100 44€

20x20

-50 1-nCL-1-A200 48€-100 1-nCL-1-B200 48€-150 1-nCL-1-C200 48€-200 1-nCL-1-D200 48€-500 1-nCL-1-E200 48€-1000 1-nCL-1-F200 48€-2000 1-nCL-1-G200 48€

30x30

-200 1-nCL-1-A300 54€-500 1-nCL-1-B300 54€-1000 1-nCL-1-C300 54€-3000 1-nCL-1-D300 54€

uvFS

10x10

-50 1-nCL-2-A100 62€-100 1-nCL-2-B100 62€-175 1-nCL-2-C100 62€-200 1-nCL-2-D100 62€-500 1-nCL-2-E100 62€-1000 1-nCL-2-F100 62€

20x20

-50 1-nCL-2-A200 68€-100 1-nCL-2-B200 68€-175 1-nCL-2-C200 68€-200 1-nCL-2-D200 68€-500 1-nCL-2-E200 68€-1000 1-nCL-2-F200 68€-2000 1-nCL-2-G200 68€

30x30

-200 1-nCL-2-A300 78€-500 1-nCL-2-B300 78€-1000 1-nCL-2-C300 78€-3000 1-nCL-2-D300 78€

CatalogItems

*[email protected]



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Clearaperture >90%

Chamfer 0.25mm@45°





MEnISCuSLEnSES

Positive or negative focal length lenses have different radii orcurvature on both sides whereas neutral meniscus lenses do notfocus light.Meniscus lensesareused inapplicationswheredistortion of the beam has to be reduced. They are used forfocusing beams in telescopes, collimators or condenser systems, optical transceivers or other devices. ALTECHnA provides lenseswithanti-reflectioncoating(PleaserefertotheCoatingsSection).

Description


Features

Miscellaneous

• Used in applications where reducing beam distortion is important

• CustomradiiofcurvatureROCavailableonrequest• variousARcoatingsareavailableforalltheselenses.PleaserefertotheCoatingsSection

• Manylensesareavailablefromourstockforattractiveprice• Customdesignproductionisalsoavailable• Massproductioncapabilities:10’000piecespermonth• variousdielectriccoatingscanbedepositedontheselenses• Checkonlinestockforattractivepricesandfastestdelivery


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• 4SCML-2-self-centering lens/opticsmount(page211)


Material Diameter,mm ROC1,mm ROC2,mm ProductID Price*l-9pcs

BK7

25.4 +50 -50 1-ML-1-A254 34€25.4 +100 -100 1-ML-1-B254 34€25.4 +150 -150 1-ML-1-C254 34€25.4 +200 -200 1-ML-1-D254 34€25.4 +250 -250 1-ML-1-E254 34€25.4 +300 -300 1-ML-1-F254 34€

uvFS

25.4 +50 -50 1-ML-2-A254 58€25.4 +100 -100 1-ML-2-B254 58€25.4 +150 -150 1-ML-2-C254 58€25.4 +200 -200 1-ML-2-D254 58€25.4 +250 -250 1-ML-2-E254 58€25.4 +300 -300 1-ML-2-F254 58€

CatalogItems

*[email protected]




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MaterialAll type of material are available to designthe optimal achromats




Clearaperture >90%

Chamfer 0.25mm@45°



ARcoatings vISornIR

ACHROMATICLEnSES

Compoundlenssystemthatformsanimagefreefromchromaticaberration. Cemented achromatic lenses significantly reducecoma and chromatic aberration. Best used to replace singlecomponents where performance must be improved.

Description


Features

Miscellaneous

• Used in applications to reduce beam distortion• variousdielectriccoatingscanbedepositedontheselenses

• Customdesignproductionisavailable• Massproductioncapabilities:4’000piecespermonth• Other dimensions are available in small and mass production

quantities


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• 4SCML-12-self-centeringlens/opticsmount(page211)

• Opticalcoatings(pages86-98)• Plano-Convexlenses(page20)


Diameter,mm

Focal length,

mm

Optimal wavelength range, nm

ARcoating ProductIDPrice

*l-9pcs

12.7 +30 400-700 vIS(400-700nm) 1-AL-1-A127-[7A00] 85€12.7 +50 400-700 vIS(400-700nm) 1-AL-1-B127-[7A00] 85€12.7 +75 400-700 vIS(400-700nm) 1-AL-1-C127-[7A00] 85€25.4 +100 400-700 vIS(400-700nm) 1-AL-1-A254-[7A00] 105€25.4 +125 400-700 vIS(400-700nm) 1-AL-1-B254-[7A00] 105€25.4 +150 400-700 vIS(400-700nm) 1-AL-1-C254-[7A00] 105€25.4 +200 400-700 vIS(400-700nm) 1-AL-1-D254-[7A00] 105€25.4 +250 400-700 vIS(400-700nm) 1-AL-1-E254-[7A00] 105€25.4 +300 400-700 vIS(400-700nm) 1-AL-1-F254-[7A00] 105€12.7 -50 400-700 vIS(400-700nm) 1-AL-1-D127-[7A00] 90€12.7 -75 400-700 vIS(400-700nm) 1-AL-1-E127-[7A00] 90€12.7 -100 400-700 vIS(400-700nm) 1-AL-1-F127-[7A00] 90€25.4 -150 400-700 vIS(400-700nm) 1-AL-1-G254-[7A00] 110€25.4 -200 400-700 vIS(400-700nm) 1-AL-1-H254-[7A00] 110€25.4 -250 400-700 vIS(400-700nm) 1-AL-1-J254-[7A00] 110€

12.7 +30 700-1050 nIR(700-1050nm) 1-AL-2-A127-[7B00] 95€12.7 +50 700-1050 nIR(700-1050nm) 1-AL-2-B127-[7B00] 95€12.7 +75 700-1050 nIR(700-1050nm) 1-AL-2-C127-[7B00] 95€25.4 +100 700-1050 nIR(700-1050nm) 1-AL-2-A254-[7B00] 125€25.4 +125 700-1050 nIR(700-1050nm) 1-AL-2-B254-[7B00] 125€25.4 +150 700-1050 nIR(700-1050nm) 1-AL-2-C254-[7B00] 125€25.4 +200 700-1050 nIR(700-1050nm) 1-AL-2-D254-[7B00] 125€25.4 +250 700-1050 nIR(700-1050nm) 1-AL-2-E254-[7B00] 125€25.4 +300 700-1050 nIR(700-1050nm) 1-AL-2-F254-[7B00] 125€12.7 -50 700-1050 nIR(700-1050nm) 1-AL-2-D127-[7B00] 100€12.7 -75 700-1050 nIR(700-1050nm) 1-AL-2-E127-[7B00] 100€12.7 -100 700-1050 nIR(700-1050nm) 1-AL-2-F127-[7B00] 100€25.4 -150 700-1050 nIR(700-1050nm) 1-AL-2-G254-[7B00] 135€25.4 -200 700-1050 nIR(700-1050nm) 1-AL-2-H254-[7B00] 135€25.4 -250 700-1050 nIR(700-1050nm) 1-AL-2-J254-[7B00] 135€

CatalogItems

*[email protected]



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LEnSCASE

ALTECHnApresentsLensCaseof22uvFSlenses.Itwillbecomean irreplaceable tool in your day to day research activities.

Description


Features

•22mounteduvFSlenses•Black25,4mmanodizedmetalrings•Epoxyfreeconfiguration(highLIDT )•ARcoatingoption•Modernsafetycasepackaging• Fast delivery

F=+,mm F=–,mm

1 35 302 50 403 60 504 75 605 100 806 125 1007 150 1508 200 2009 300 30010 500 50011 750 12 1000

Price(foruncoatedlensesinLensCase) 990€*Clearaperture:>18mm

LensCasecontainsfollowinguvFSPlano–Convex&Plano–Concavelenses*

MountDiameter 25,4mm+0.00/-0.2mm

Focal length tolerance +/-2%


Clearaperture >18mm





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•Plano-Convexlenses(page20)

•Plano-Concavelenses(page23)

BroadbandARcoatedlensesinLensCase

Wavelength, nm Residualreflectivity,% Priceofcoatedset266-370 <0,5 1.430€400-700 <1,0 1.430€600-1050 <0,8 1.430€700-950 <0,4 1.430€750-850 <0,3 1.430€750-1000 <0,5 1.430€900-1200 <0,6 1.430€1200-1500 <0,6 1.430€1500-1900 <0,7 1.430€

DualARcoatedlensesinLensCase

Wavelength, nm Residualreflectivity,% Priceofcoatedset266+532 <0,5 1.290€343+1030 <0,3 1.290€355+532 <0,3 1.290€355+1064 <0,3 1.290€399+556 <0,3 1.290€400+800 <0,3 1.290€426+852 <0,3 1.290€515+1030 <0,25 1.290€532+1064 <0,25 1.290€1064+1319 <0,3 1.290€

LaserlineARcoatedlensesinLensCase

Wavelength, nm Residualreflectivity,% Priceofcoatedset266 <0,5 1.250€

343-355 <0,25 1.250€400 <0,2 1.250€

473-488 <0,2 1.250€515 <0,2 1.250€

527 - 532 <0,2 1.250€589 <0,2 1.250€633 <0,2 1.250€780 <0,2 1.250€800 <0,2 1.250€852 <0,2 1.250€946 <0,2 1.250€980 <0,2 1.250€1030 <0,2 1.250€

1047-1064 <0,2 1.250€1122 <0,2 1.250€1319 <0,2 1.250€1550 <0,2 1.250€


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Material BK7,uvFS


Apexangle 90–179.98°

Clearaperture >90%

Apexangletolerance ±0.5°.Availabledownto+/-0.02°




PLAnO-COnvEXAXICOnS(ConiCal lenses)

Plano-convex axicons are conical lenses which are used forvariety of applications. When followed by a conventional spherical lens, axicons can focus laser light to a ring shapewith annular focus. This feature can be used in hole drilling,microscopy and medical applications. Another interesting feature of axicons is a possibility to transform Gaussian beamintonon-diffractiveBesselbeaminthenearfield.Besselbeamscan be used in atom or molecule guiding applications.

Altechnaofferstwotypesofplano-convexaxicons: regularandprecision. Regular axicons will create annularly shaped beamwhereas precision axicons will also transform Gaussian beaminto aBesselbeam.youcanchooseaccordingly,depending toyour specific application.

Description


Features

Miscellaneous

• ProducesnondiffractingBesselbeaminthenearfieldandring shaped image in the far field

• Availablediameterupto50mm• Planoconvex,planoconcaveanddoubleconvexavailable• variousARcoatingsareavailableforalltheselenses.PleaserefertotheCoatingsSection

• Customdesignproductionisavailable• Massproductioncapabilities:4’000piecespermonth


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• 4SCLM-2-self-centeringlens/opticsmount(page211)

Material Diameter,mm Apexangle,˚ ProductID Price*l-9pcs

BK7

25.4 90 1-APX-1-A254 260€25.4 130 1-APX-1-B254 235€25.4 140 1-APX-1-C254 235€25.4 160 1-APX-1-D254 235€25.4 170 1-APX-1-E254 235€25.4 175 1-APX-1-F254 235€25.4 176 1-APX-1-G254 235€25.4 178 1-APX-1-H254 235€25.4 179 1-APX-1-J254 235€

uvFS

25.4 90 1-APX-2-A254 305€25.4 130 1-APX-2-B254 290€25.4 140 1-APX-2-C254 290€25.4 160 1-APX-2-D254 290€25.4 170 1-APX-2-E254 290€25.4 175 1-APX-2-F254 290€25.4 176 1-APX-2-G254 290€25.4 178 1-APX-2-H254 290€25.4 179 1-APX-2-J254 290€

CatalogItems

*[email protected]


HOWTOREQuEST/ORDERCOATEDELEMEnT:

variouscoatingsareavailableontheseelements.Please

refertotheCoatingsSectionforthestandardcoatings.If

youwanttoorderAR/AR@532nmcoatedaxiconyou

can simplymodify the Product ID by adding standard

coating code in the brackets as following:

• 5KOM4-1–fouraxiskinematicopticalmount(page229)

PRECISIOnPCXAXICOnS


uvFS

25.4 130 1-APX-2-B254-P 640€25.4 140 1-APX-2-C254-P 640€25.4 160 1-APX-2-D254-P 640€25.4 170 1-APX-2-E254-P 640€25.4 175 1-APX-2-F254-P 640€25.4 176 1-APX-2-G254-P 640€25.4 178 1-APX-2-H254-P 640€25.4 179 1-APX-2-J254-P 640€

• Beamexpander(page186)


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Material BK7,uvFS


Apexangle 90–179.98˚

Clearaperture >90%

Apexangletolerance ±0.5˚.AvailableDownto±0.02˚




PLAnO-COnCAvEAXICOnS(ConiCal lenses)

Plano-concave axicons have a plano surface in combinationwith a concave conical surface. Concave axicon produces aringshapedimagealongtheaxisfromapointlightsource(e.g.Gaussian laserbeam).Due to specifics in fabricationprocess, ahole in the center of concave surface is needed. Diameter oftheholeistypically1mm.Differentcoatingscanbeappliedonthe polished surfaces of axicons (please refer to the coatingssection in page XX). When coated with HR coating, concaveconical surface can be used as a conical mirror in some specific applications.

Description


Features

Miscellaneous

• Producesaringshapedimagealongtheaxisfromapointlight source

• Availablediameterupto50mm• variousARcoatingsareavailableforalltheselenses.PleaserefertotheCoatingsSection

•Customdesignproductionisavailable


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BK7

25.4 90 1-APC-1-A254 495€25.4 130 1-APC-1-B254 415€25.4 140 1-APC-1-C254 415€25.4 160 1-APC-1-D254 415€25.4 170 1-APC-1-E254 415€25.4 175 1-APC-1-F254 415€25.4 176 1-APC-1-G254 415€25.4 178 1-APC-1-H254 415€25.4 179 1-APC-1-J254 415€

uvFS

25.4 90 1-APC-2-A254 520€25.4 130 1-APC-2-B254 465€25.4 140 1-APC-2-C254 465€25.4 160 1-APC-2-D254 465€25.4 170 1-APC-2-E254 465€25.4 175 1-APC-2-F254 465€25.4 176 1-APC-2-G254 465€25.4 178 1-APC-2-H254 465€25.4 179 1-APC-2-J254 465€

CatalogItems

*[email protected]


• 5TLM-1-y-Zpositionerforlens,pinholesandobjectives(page230)

• Beamexpander(page186)

• 4OCM-25–opticalcomponentmount(page212)


variouscoatingsareavailableontheseelements.Please

refertotheCoatingsSectionforthestandardcoatings.If

youwanttoorderAR/AR@532nmcoatedaxiconyou

can simplymodify the Product ID by adding standard

coating code in the brackets as following:


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Material BK7,uvFS


Apexangle 90–179.98˚

Clearaperture >90%

Apexangletolerance ±0.5˚.Availabledownto±0.02˚



Available focal length 20-10000mm

Radiustolerance ±3%


DOuBLECOnvEXAXICOnS(ConiCal lenses)

Double convex axicons are available in variety of dimensionsandapexangles.Doubleconvexaxiconsareopticalcomponentswith a convex conical surface in combination with a convexspherical surface. Such combination focuses laser light into a ringshapedbeamwithannularfocus.Differentcombinationsoffocallengthandapexanglesareavailable.

Description


Features

• Used in applications to reduce beam distortion• Other dimensions are available in small and mass production

quantities• variousARcoatingsareavailableforalltheselenses.PleaserefertotheCoatingsSection

• Massproductioncapabilities:100piecespermonth


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• 5TLM-1-y-Zpositionerforlens,pinholesandobjectives(page230)

MaterialDiameter,

mm

Focal Length Rangeofthe

Spherical Face, mm

ApexAngle,˚

ProductidPrice

1-5Pcs*

BK7

25.4 50-2000 90 1-ADX-1-A254 600€25.4 50-2000 130 1-ADX-1-B254 580€25.4 50-2000 140 1-ADX-1-C254 580€25.4 50-2000 160 1-ADX-1-D254 580€25.4 50-2000 170 1-ADX-1-E254 580€25.4 50-2000 175 1-ADX-1-F254 580€25.4 50-2000 176 1-ADX-1-G254 580€25.4 50-2000 178 1-ADX-1-H254 580€25.4 50-2000 179 1-ADX-1-J254 580€

uvFS

25.4 50-2000 90 1-ADX-2-A254 780€25.4 50-2000 130 1-ADX-2-B254 740€25.4 50-2000 140 1-ADX-2-C254 740€25.4 50-2000 160 1-ADX-2-D254 740€25.4 50-2000 170 1-ADX-2-E254 740€25.4 50-2000 175 1-ADX-2-F254 740€25.4 50-2000 176 1-ADX-2-G254 740€25.4 50-2000 178 1-ADX-2-H254 740€25.4 50-2000 179 1-ADX-2-J254 740€

CatalogItems

*[email protected]



variouscoatingsareavailableontheseelements.PleaserefertotheCoatingsSectionforthe

standardcoatings.IfyouwanttoorderAR/AR@532nmcoatedaxiconyoucansimplymodify

theProductIDbyaddingstandardcoatingcodeinthebracketsasfollowing:

• Plano-Convexlenses(page20)• Plano-Concavelenses(page23)

• Opticalcoatings(pages86-98)• Beamexpander(page186)


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Material BK7,uvFS,IRFS

Dimensiontolerances +0.00/-0.2mm


Flatness λ/[email protected]

Angle tolerance ±2arcmin

Designwavelength 780nm

Coatings none.PleaserefertoCoatingsSection

DISPERSInGPRISMS

Dispersing prisms are used for wavelength separationapplications. A light ray is twice refracted passing through the prism. Deviation is a function of refractive index, and hencewavelength.

Description


Features

Miscellaneous

• Separates light by wavelength

•Customdesignproductionavailable•variousdielectriccoatingscanbedepositedonrequest• We can make the prisms from other material


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Material DimensionsAxL,mm Coating ProductIDPrice

*1-5pcs

BK712,5x12,5 Uncoated 1-PD-1-0125 42€25x25 Uncoated 1-PD-1-0250 56€

uvFS12,5x12,5 Uncoated 1-PD-2-0125 68€25x25 Uncoated 1-PD-2-0250 86€

CatalogItems


variouscoatingsareavailableontheseelements.PleaserefertotheCoatingsSectionforthe

standardcoatings.IfyouwanttoorderAR/AR@532nmcoatedprismyoucansimplymodify

theProductIDbyaddingstandardcoatingcodeinthebracketsasfollowing:

*[email protected]


• 5PM131-prism/opticsmount(page231)


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Material BK7,IRFS,uvFS

Dimensiontolerances +0.00/-0,2mm


Clearaperture 80%ofthefacesize


90˚angletolerance±2arcmin(Generaltype)±5arcsec(Precisiontype)

Pyramidaltolerance±1arcmin(Generaltype)±30arcsec(Precisiontype)


RIGHT-AnGLEPRISMS

Right angle prisms are used to direct beams at 90 degrees byusing the hypotenuse face for total internal reflection (TIR).These prisms are often preferable to an inclined mirror inapplications involving severe acoustic or inertial loads, because they are easier to mount, and deform much less than mirrors in response to externalmechanical stress. As long as acceptanceangle limitations forTIR from the roof faces are not exceeded,the right angle prism can also serve as a retroreflector, reflecting a beam back.

Description


Features

Miscellaneous

•Canworkasinternalorexternalreflectorsorasretro-reflectors

• Customdesignproductionisalsoavailable• variousdielectriccoatingscanbedepositedonthese

elements on request• We can make the prisms from other material on your needs


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Relatedproductsandaccessories• 5OM37-50-twoangularfineadjustmentmounts(page223)

• 7FA3–roll&pitchtiltplatform(page233)

Material DimensionsAxBxC,mm Angle tolerance ProductIDPrice

*1-5pcs

BK7

12.5x12.5x12.5Generaltype 1-PR-1-0125 16€Precisiontype 1-PR-1-1125 38€



uvFS




CatalogItems

*[email protected]


• 5PM57-prism/opticsmount(page225)

• 5PMF57-universalprism/opticsmount(page225)

• 6PT169-threeangleprism/beamsplit-tertable(page232)

• Cornercuberetroreflectors(page51)• Opticalcoatings(pages86-98)


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Material BK7



Clearaperture 80%ofthefacesize


90˚angletolerance ±2arcmin(Generaltype)


RIGHT-AnGLEPRISMSRETROREFLECTORS

Right-angle prisms retroreflectors are often preferable to aninclined mirror in applications involving severe acoustic or inertial loads, because they are easier to mount, and deform muchlessthanamirrorinresponsetoexternalmechanicalstress.As long as acceptance angle limitations for TIR from the rooffaces are not exceeded, the prism is working as retroreflector,reflecting a beam back.

Description


Features

• Worksasinternalretro-reflectororexternalreflector

CatalogItems

Material DimensionsLxHxT,mm ProductID Price

BK7

16x10x5 1-PRR-1-0016 72€18x8x4 1-PRR-1-0018 72€22x16x8 1-PRR-1-0022 78€25x10x4 1-PRR-1-0025 78€35x10x5 1-PRR-1-0035 94€


•6PT110–tilt/rotationstage(page232)

•Cornercuberetroreflectors(page51)•Opticalcoatings(pages86-98)

Miscellaneous

• Customdesignproductionisavailable• variousdielectriccoatingscanbedepositedonrequest• We can make the prisms from other material based on your

needs


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Material BK7,uvFS




Beamdeviation 180°±30arcsec

Angular deviation ±5arcsec

CORnERCuBERETROREFLECTORS

Corner cube retroreflectors are designed to deviate incidentlight by 180 degrees independent of the angle of incidence.Theseprismshave3mirrorsurfacesmakinganglesof90degreesto each other, juxtaposed to form the corner of a cube withthe entrance face perpendicular to cube diagonal. All beams, independent of the direction of incidence, are reflected back. Corner cubes are used for high precision applications or withlasers working in very long distances.

Description

Standard Specifications

Features

Miscellaneous

• Incidentlightdeviatesby180˚reesindependentlyoftheangle of incidence

• Mainlyusedinhighprecisionapplicationsorwithlasersworking in very long distances

• Customdesignproductionisavailable• variousdielectriccoatingscanbedepositedonrequest• We can make the prisms from other material based on

your needs. • Higherangletoleranceprecisionisalsoavailable

CatalogItems

MaterialDimensionsdxh,

mmCoating ProductID Price

BK725.4x19.0 Uncoated 1-PCR-1-0254 96€38.1x28.5 Uncoated 1-PCR-1-0381 126€

uvFS 25.4x19.0 Uncoated 1-PCR-2-0254 172€



• Right-Angleprisms(page48)• Opticalcoatings(pages86-98)


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Substrate dimension tolerance +0.00/-0.1mm

Substrate wavefront distortion <λ/8(<λ/4forcurvedsurfaces)

Substrate surface quality20-10Scratch&Dig(40-20Scratch&Digforcurvedsurfaces)

Coatingadhesionanddurability PerMIL-C-675A

Clearaperture >90%ofdiameter

MeasuredreflectivityR>99.5%@0°, Rs>99.8%andRp>99.3%@45°

Laser damage threshold >5-7J/cm2for10nspulses@1064nm

HRLASERLInEMIRRORS(HR)

HR laser line mirrors (HR) provide optimized performance atcertainwavelengthandcertainangleof incidence(AOI).Mirrorconsists of substrate and multilayer coating stacks which help to achieve very high reflectivity at specific laser line wavelength at anydesignedangleofincidence.LaserlineHRcoatingsareusedforexternalbeammanipulationapplicationswhereevenslightlossesmay be intolerable. Coatings are provided by Ion BeamSputtering(IBS)orelectronbeamevaporationwith/withoutionassistance coating techniques.

Highreflectivitydielectriccoatingsintherangeof0.19-20μmare available.

Description


Features

Miscellaneous

• Provideanoptimisedperformanceatcertainwavelengthandcertainangleofincidence(AOI)

• variousdimensionsareavailableinsmallandmassproduction quantities

• Massproductioncapabilities:1’000piecespermonth

• Coatingsareprovidedbyionbeamsputtering(IBS)orelectron beam evaporation with/without ion assistance coating techniques.

• HRlaserlinecoatings(HR)highlyreflectwavelengthrangeof<10%ofthecentralwavelength(CWL).Forinstance,HR@800nmwillreflectwavelengthrangeof760-840nm.

• Ifyourapplicationneedstoreflectwiderwavelengthrangepleasereferto-BroadBandHRwavelength(BBHR)coatings.

Measuredtransmissioncurveofthestandardcoatingcode1E45


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Wavelength, nm

Reflectivity(average),

%

Substrate material

ProductIDforAOI=0°

ProductIDforAOI=45°

Price*1-6pcs

ProductIDforAOI=0°


Price*1-6pcs

Ø12.7mm Ø25.4mm266 >99.0 uvFS 1-OS-2-0127-2-[1A00] 1-OS-2-0127-2-[1A45] 67€ 1-OS-2-0254-5-[1A00] 1-OS-2-0254-5-[1A45] 75€

343-355 >99.5 uvFS 1-OS-2-0127-2-[1B00] 1-OS-2-0127-2-[1B45] 67€ 1-OS-2-0254-5-[1B00] 1-OS-2-0254-5-[1B45] 75€

400 >99.5 uvFS 1-OS-2-0127-2-[1C00] 1-OS-2-0127-2-[1C45] 51€ 1-OS-2-0254-5-[1C00] 1-OS-2-0254-5-[1C45] 59€

473-488 >99.5 BK7 1-OS-1-0127-3-[1D00] 1-OS-1-0127-3-[1D45] 45€ 1-OS-1-0254-6-[1D00] 1-OS-1-0254-6-[1D45] 51€

515 >99.5 uvFS 1-OS-2-0127-2-[1E00] 1-OS-2-0127-2-[1E45] 51€ 1-OS-2-0254-5-[1E00] 1-OS-2-0254-5-[1E45] 59€

527 - 532 >99.5 BK7 1-OS-1-0127-3-[1F00] 1-OS-1-0127-3-[1F45] 45€ 1-OS-1-0254-6-[1F00] 1-OS-1-0254-6-[1F45] 51€

589 >99.5 BK7 1-OS-1-0127-3-[1G00] 1-OS-1-0127-3-[1G45] 45€ 1-OS-1-0254-6-[1G00] 1-OS-1-0254-6-[1G45] 51€

633 >99.5 BK7 1-OS-1-0127-3-[1H00] 1-OS-1-0127-3-[1H45] 45€ 1-OS-1-0254-6-[1H00] 1-OS-1-0254-6-[1H45] 51€

780 >99.5 uvFS 1-OS-2-0127-2-[1J00] 1-OS-2-0127-2-[1J45] 51€ 1-OS-2-0254-5-[1J00] 1-OS-2-0254-5-[1J45] 59€

800 >99.5 uvFS 1-OS-2-0127-2-[1K00] 1-OS-2-0127-2-[1K45] 51€ 1-OS-2-0254-5-[1K00] 1-OS-2-0254-5-[1K45] 59€

852 >99.5 BK7 1-OS-1-0127-3-[1L00] 1-OS-1-0127-3-[1L45] 45€ 1-OS-1-0254-6-[1L00] 1-OS-1-0254-6-[1L45] 51€

946 >99.5 BK7 1-OS-1-0127-3-[1M00] 1-OS-1-0127-3-[1M45] 45€ 1-OS-1-0254-6-[1M00] 1-OS-1-0254-6-[1M45] 51€

980 >99.5 BK7 1-OS-1-0127-3-[1n00] 1-OS-1-0127-3-[1n45] 45€ 1-OS-1-0254-6-[1n00] 1-OS-1-0254-6-[1n45] 51€

1030 >99.5 uvFS 1-OS-2-0127-2-[1P00] 1-OS-2-0127-2-[1P45] 51€ 1-OS-2-0254-5-[1P00] 1-OS-2-0254-5-[1P45] 59€

1047-1064 >99.5 BK7 1-OS-1-0127-3-[1R00] 1-OS-1-0127-3-[1R45] 45€ 1-OS-1-0254-6-[1R00] 1-OS-1-0254-6-[1R45] 51€

1122 >99.5 BK7 1-OS-1-0127-3-[1S00] 1-OS-1-0127-3-[1S45] 45€ 1-OS-1-0254-6-[1S00] 1-OS-1-0254-6-[1S45] 51€

1319 >99.5 BK7 1-OS-1-0127-3-[1T00] 1-OS-1-0127-3-[1T45] 61€ 1-OS-1-0254-6-[1T00] 1-OS-1-0254-6-[1T45] 67€

1550 >99.5 BK7 1-OS-1-0127-3-[1v00] 1-OS-1-0127-3-[1v45] 61€ 1-OS-1-0254-6-[1v00] 1-OS-1-0254-6-[1v45] 67€

CatalogItems


• Opticalsubstrates(page18)• HRbroadbandmirrors(BBHR)(page54)• 5F21-1 - flipping mirror/ beamsplitter mount(page217)

• 5KvDOM-1-kinematicverticaldriveopti-calmount(page216)

• 5MBM24-2-2SQ-kinematicmirror/beamsplittermount(page224)

pLeASe noTe:thicknessofuvFSØ12.7mmis2mm;thicknessofBK7Ø12.7mmis3mmthicknessofuvFSØ25.4mmis5mm;thicknessofBK7Ø25.4mmis6mm•IfyoudonotfindsuitablewavelengthorAOIforyourapplicationpleasecontactusandwewillprovidethebestsolutionforyou!•Anyofourstandardsubstratescanbecoatedwiththesetypesofcoatings!•Curvedsubstratescanalsobecoated!

HRlaserlinemirrors(HR)


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Measuredreflectivity R>99%@0°,Rave>99%@45°


HRBROADBAnDMIRRORS(BBHR)

HR broad band mirrors (BBHR) provide high reflectivity for abroad spectrum.Therefore, it is ideal solution for awide rangeofmulti-wavelength laser orwhite light applications. Coatingsare provided by Ion Beam Sputtering (IBS) or electron beamevaporation with/without ion assistance coating techniques.


Description


Features

Miscellaneous

• Providesoptimisedperformanceatcertainwavelengthandcertainangleofincidence(AOI)

• Other dimensions are available in small and mass production quantities



• Ifyourapplicationdoesnotrequiresuchawidewavelengthrangepleasereferto-HRlaserlinemirrors

Measuredtransmissioncurveofthestandardcoatingcode2C00


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Wavelength range, nm

Reflectivity(average),

%

Substrate material

ProductIDforAOI=0°


Price*1-6 pcs

ProductIDforAOI=0°


Price*1-6 pcs

Ø12.7x3mm Ø25.4x6mm400-700 >99.0 BK7 1-OS-1-0127-3-[2A00] 1-OS-1-0127-3-[2A45] 74€ 1-OS-1-0254-6-[2A00] 1-OS-1-0254-6-[2A45] 92€700-950 >99.0 BK7 1-OS-1-0127-3-[2B00] 1-OS-1-0127-3-[2B45] 74€ 1-OS-1-0254-6-[2B00] 1-OS-1-0254-6-[2B45] 92€750-850 >99.0 BK7 1-OS-1-0127-3-[2C00] 1-OS-1-0127-3-[2C45] 74€ 1-OS-1-0254-6-[2C00] 1-OS-1-0254-6-[2C45] 92€750-1000 >99.0 BK7 1-OS-1-0127-3-[2D00] 1-OS-1-0127-3-[2D45] 74€ 1-OS-1-0254-6-[2D00] 1-OS-1-0254-6-[2D45] 92€900-1200 >99.0 BK7 1-OS-1-0127-3-[2E00] 1-OS-1-0127-3-[2E45] 74€ 1-OS-1-0254-6-[2E00] 1-OS-1-0254-6-[2E45] 92€

CatalogItems

•IfyoudonotfindsuitablewavelengthorAOIforyourapplicationpleasecontactusandwewillprovidethebestsolutionforyou!•Any of our standard substrates can be coated with these types of coatings•Curvedsubstratescanalsobecoated

HRbroadbandmirrors(BBHR)


• 5F23-05-miniatureflippingmirror/beamsplittermounts(page217)

• 5MBM23-05-3SH - miniature kinematic mirror/beamsplittermount(page225)


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Coatingadhesionanddurability PerMIL-C-675A.



PARTIALREFLECTInGMIRRORS(PR)

Partial reflecting mirrors (PR) provide required percentagereflection/transmission at specific angle of incidence for both singleandbroadbandwavelengths.Thesecoatingsareusuallyused for efficient beam splitting as well as output coupling in high power laser cavities.

Description


Features

Miscellaneous

• Efficientbeamsplittingaswellasoutputcouplinginhighpower laser cavities


• Massproductioncapabilities:1’000piecespermonth• variouswavelengthsandreflectivityvaluesareavailable


Relatedproductsandaccessories• Opticalsubstrates(page18)• 5OM10T-smallopticalmountofsidedrivewithmirroradapter5OM100A3(page226)

• 5M111-0–mirror/opticsmount • 5BM57-2-stablesteelmirror/beamsplittermounts(page223)

MeasuredtransmissioncurveforPRcoatingcode3F00-50


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Wavelength, nm

Substrate material

Reflectivity(s-pol),%

ProductIDforAOI=0°


Price*1-6 pcs

ProductIDforAOI=0°


Price*1-6 pcs

Ø12.7mm Ø25.4mm

266 uvFS10±3 1-OS-2-0127-2-[3A00-10] 1-OS-2-0127-2-[3A45-10] 87€ 1-OS-2-0254-5-[3A00-10] 1-OS-2-0254-5-[3A45-10] 97€50±2 1-OS-2-0127-2-[3A00-50] 1-OS-2-0127-2-[3A45-50] 87€ 1-OS-2-0254-5-[3A00-50] 1-OS-2-0254-5-[3A45-50] 97€90±1 1-OS-2-0127-2-[3A00-90] 1-OS-2-0127-2-[3A45-90] 87€ 1-OS-2-0254-5-[3A00-90] 1-OS-2-0254-5-[3A45-90] 97€

355 uvFS10±3 1-OS-2-0127-2-[3B00-10] 1-OS-2-0127-2-[3B45-10] 87€ 1-OS-2-0254-5-[3B00-10] 1-OS-2-0254-5-[3B45-10] 97€50±2 1-OS-2-0127-2-[3B00-50] 1-OS-2-0127-2-[3B45-50] 87€ 1-OS-2-0254-5-[3B00-50] 1-OS-2-0254-5-[3B45-50] 97€90±1 1-OS-2-0127-2-[3B00-90] 1-OS-2-0127-2-[3B45-90] 87€ 1-OS-2-0254-5-[3B00-90] 1-OS-2-0254-5-[3B45-90] 97€

400 uvFS10±3 1-OS-2-0127-2-[3C00-10] 1-OS-2-0127-2-[3C45-10] 87€ 1-OS-2-0254-5-[3C00-10] 1-OS-2-0254-5-[3C45-10] 97€50±2 1-OS-2-0127-2-[3C00-50] 1-OS-2-0127-2-[3C45-50] 87€ 1-OS-2-0254-5-[3C00-50] 1-OS-2-0254-5-[3C45-50] 97€90±1 1-OS-2-0127-2-[3C00-90] 1-OS-2-0127-2-[3C45-90] 87€ 1-OS-2-0254-5-[3C00-90] 1-OS-2-0254-5-[3C45-90] 97€

515 - 532 BK710±3 1-OS-1-0127-3-[3D00-10] 1-OS-1-0127-3-[3D45-10] 79€ 1-OS-1-0254-6-[3D00-10] 1-OS-1-0254-6-[3D45-10] 87€50±2 1-OS-1-0127-3-[3D00-50] 1-OS-1-0127-3-[3D45-50] 79€ 1-OS-1-0254-6-[3D00-50] 1-OS-1-0254-6-[3D45-50] 87€90±1 1-OS-1-0127-3-[3D00-90] 1-OS-1-0127-3-[3D45-90] 79€ 1-OS-1-0254-6-[3D00-90] 1-OS-1-0254-6-[3D45-90] 87€

633 BK710±3 1-OS-1-0127-3-[3E00-10] 1-OS-1-0127-3-[3E45-10] 79€ 1-OS-1-0254-6-[3E00-10] 1-OS-1-0254-6-[3E45-10] 87€50±2 1-OS-1-0127-3-[3E00-50] 1-OS-1-0127-3-[3E45-50] 79€ 1-OS-1-0254-6-[3E00-50] 1-OS-1-0254-6-[3E45-50] 87€90±1 1-OS-1-0127-3-[3E00-90] 1-OS-1-0127-3-[3E45-90] 79€ 1-OS-1-0254-6-[3E00-90] 1-OS-1-0254-6-[3E45-90] 87€

750-850 uvFS10±3 1-OS-2-0127-2-[3F00-10] 1-OS-2-0127-2-[3F45-10] 87€ 1-OS-2-0254-5-[3F00-10] 1-OS-2-0254-5-[3F45-10] 97€50±2 1-OS-2-0127-2-[3F00-50] 1-OS-2-0127-2-[3F45-50] 87€ 1-OS-2-0254-5-[3F00-50] 1-OS-2-0254-5-[3F45-50] 97€90±1 1-OS-2-0127-2-[3F00-90] 1-OS-2-0127-2-[3F45-90] 87€ 1-OS-2-0254-5-[3F00-90] 1-OS-2-0254-5-[3F45-90] 97€

946 BK710±3 1-OS-1-0127-3-[3G00-10] 1-OS-1-0127-3-[3G45-10] 79€ 1-OS-1-0254-6-[3G00-10] 1-OS-1-0254-6-[3G45-10] 87€50±2 1-OS-1-0127-3-[3G00-50] 1-OS-1-0127-3-[3G45-50] 79€ 1-OS-1-0254-6-[3G00-50] 1-OS-1-0254-6-[3G45-50] 87€90±1 1-OS-1-0127-3-[3G00-90] 1-OS-1-0127-3-[3G45-90] 79€ 1-OS-1-0254-6-[3G00-90] 1-OS-1-0254-6-[3G45-90] 87€

1020-1100 BK710±3 1-OS-1-0127-3-[3H00-10] 1-OS-1-0127-3-[3H45-10] 79€ 1-OS-1-0254-6-[3H00-10] 1-OS-1-0254-6-[3H45-10] 87€50±2 1-OS-1-0127-3-[3H00-50] 1-OS-1-0127-3-[3H45-50] 79€ 1-OS-1-0254-6-[3H00-50] 1-OS-1-0254-6-[3H45-50] 87€90±1 1-OS-1-0127-3-[3H00-90] 1-OS-1-0127-3-[3H45-90] 79€ 1-OS-1-0254-6-[3H00-90] 1-OS-1-0254-6-[3H45-90] 87€

1122 BK710±3 1-OS-1-0127-3-[3J00-10] 1-OS-1-0127-3-[3J45-10] 79€ 1-OS-1-0254-6-[3J00-10] 1-OS-1-0254-6-[3J45-10] 87€

50±2 1-OS-1-0127-3-[3J00-50] 1-OS-1-0127-3-[3J45-50] 79€ 1-OS-1-0254-6-[3J00-50] 1-OS-1-0254-6-[3J45-50] 87€90±1 1-OS-1-0127-3-[3J00-90] 1-OS-1-0127-3-[3J45-90] 79€ 1-OS-1-0254-6-[3J00-90] 1-OS-1-0254-6-[3J45-90] 87€

1319 BK710±3 1-OS-1-0127-3-[3K00-10] 1-OS-1-0127-3-[3K45-10] 79€ 1-OS-1-0254-6-[3K00-10] 1-OS-1-0254-6-[3K45-10] 87€50±2 1-OS-1-0127-3-[3K00-50] 1-OS-1-0127-3-[3K45-50] 79€ 1-OS-1-0254-6-[3K00-50] 1-OS-1-0254-6-[3K45-50] 87€90±1 1-OS-1-0127-3-[3K00-90] 1-OS-1-0127-3-[3K45-90] 79€ 1-OS-1-0254-6-[3K00-90] 1-OS-1-0254-6-[3K45-90] 87€

1550 BK710±3 1-OS-1-0127-3-[3L00-10] 1-OS-1-0127-3-[3L45-10] 79€ 1-OS-1-0254-6-[3L00-10] 1-OS-1-0254-6-[3L45-10] 87€50±2 1-OS-1-0127-3-[3L00-50] 1-OS-1-0127-3-[3L45-50] 79€ 1-OS-1-0254-6-[3L00-50] 1-OS-1-0254-6-[3L45-50] 87€90±1 1-OS-1-0127-3-[3L00-90] 1-OS-1-0127-3-[3L45-90] 79€ 1-OS-1-0254-6-[3L00-90] 1-OS-1-0254-6-[3L45-90] 87€

CatalogItems

pLeASe noTe:thicknessofuvFSØ12.7mmis2mm;thicknessofBK7Ø12.7mmis3mmthicknessofuvFSØ25.4mmis5mm;thicknessofBK7Ø25.4mmis6mm•IfyoudonotfindsuitablewavelengthorAOIforyourapplicationpleasecontactusandwewillprovidethebestsolutionforyou!•Any of our standard substrates can be coated with these types of coatings•Curvedsubstratescanalsobecoated

Partialreflectingmirrors(PR)


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GTICHIRPEDMIRROR

Description

A Gires–Tournois interferometer (GTI) is an optical standing-wave resonator designed for generating chromatic dispersion. GTI mirrors are used mainly for pulse compression in yb:yAG,yb:KGW femtosecond lasers, but can be optimized for otherwavelengths,forexampleTi:Sapphirelasersystem.ComparedtoprismorgratingpulsecompressionsystemsGTIthinfilmmirrorsexhibitslowerlossesandsensitivitytomechanicalmisalignmenterrors, thus enabling higher output power and stability of laser system.


Material Fused Silica

Substrate dimension tolerance +0/-0,1mm

Substrate wavefront distortion <L/8@633nm

Surface quality 20/10S/D


Clearaperture >90%

ReflectivityRsp>99,8%@1010nm–1080nm,AOI=0°-10°Rsp>99,8%@700-900nm,AOI=0°-10°

Features

• Reflectivityupto99,9%.• Centralwavelengthtoleranceupto1%.• GDDvaluesrangesfrom100to1500fs2foryb:KGW,yb:yAG

laser type coatings according to customer specifications. • CalculatedandmeasuredGDDcurvesaresuppliedwithevery

batch.

MeasuredGDDcurveforGTImirror,HR>99.8%@700-900nm,GDD@780-820nm,AOI=0deg

MeasuredreflectioncurveforGTImirror,HR>99.8%@700-900nm,GDD@780-820nm,AOI=0deg


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Material Size, mm Wavelength range, nm AverageGDD,fs2 AOI,deg ProductIDPrice

*1-9 pcsuvFS Ø12.7x5 780-820 -150 0-10 1-OS-2-0127-5-150-[10A00] CallusuvFS Ø25.4x5 780-820 -150 0-10 1-OS-2-0254-5-150-[10A00] CallusuvFS Ø12.7x5 780-820 -250 0-10 1-OS-2-0127-5-250-[10A00] CallusuvFS Ø25.4x5 780-820 -250 0-10 1-OS-2-0254-5-250-[10A00] CallusuvFS Ø12.7x5 780-820 -400 0-10 1-OS-2-0127-5-400-[10A00] CallusuvFS Ø25.4x5 780-820 -400 0-10 1-OS-2-0254-5-400-[10A00] CallusuvFS Ø12.7x5 1020-1060 -200 0-10 1-OS-2-0127-5-200-[10B00] CallusuvFS Ø25.4x5 1020-1060 -200 0-10 1-OS-2-0254-5-200-[10B00] CallusuvFS Ø12.7x5 1020-1060 -400 0-10 1-OS-2-0127-5-400-[10B00] CallusuvFS Ø25.4x5 1020-1060 -400 0-10 1-OS-2-0254-5-400-[10B00] CallusuvFS Ø12.7x5 1020-1060 -600 0-10 1-OS-2-0127-5-600-[10B00] CallusuvFS Ø25.4x5 1020-1060 -600 0-10 1-OS-2-0254-5-600-[10B00] CallusuvFS Ø12.7x5 1020-1060 -1000 0-10 1-OS-2-0127-5-1000-[10B00] CallusuvFS Ø25.4x5 1020-1060 -1000 0-10 1-OS-2-0254-5-1000-[10B00] Callus

*Ifyoudonotfindsuitablespecifications,pleasecontactus

MeasuredGDDcurveforGTImirror,HR>99.8%@930-1150nm,GDD@1020-1060nm,OI=0deg

MeasuredreflectioncurveforGTImirror,HR>99.8%@930-1150nm,GDD@1020-1060nm,AOI=0deg

Relatedproductsandaccessories• Ti:Sapphirelasercrystal(page126) • Broadband(ultrafast)thinfilmpolarizers

(page111)• 5BM131–beamsplitter/mirrormount(page220)


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Laser damage threshold >5J/cm2for10nspulses@1064nm

WAvELEnGTHSEPARATORS

Wavelength separators are used to separate the spectral regions or specified wavelengths (harmonic components) of themulti-wavelegth laser systems by selective spectral reflection, transmission and absorption.

Wavelegth separators are used to clean second harmonic from remains of first harmonic: selected wavelegths are reflected while others are transmitted.

Description


Features

Miscellaneous

• Used to separate the spectral regions or specified wavelengths



• Coatingsareprovidedbyionbeamsputtering(IBS)orelectron beam evaporation with/without ion assistance coating techniques

• Separators for other wavelengths are available on request

Measuredtransmissioncurveforwavelengthseparatorcoatingcode4D45


• Opticalsubstrates(page18) • 5F21-1 - flipping mirror/ beamsplitter mount(page217)

• 5APH79T-1-kinematicdoubleopticalmount of side drive with adjustable polar-izerholder(page218)


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Reflectedwavelength,nm

Transmittedwavelength,nm Material Size ProductIDforAOI=0° ProductIDforAOI=45°Price

*1-6 pcs

R>99%@266 T>90%@355+532+1064 uvFSØ12.7x2mm 1-OS-2-0127-2-[4A00] 1-OS-2-0127-2-[4A45] 77€Ø25.4x5mm 1-OS-2-0254-5-[4A00] 1-OS-2-0254-5-[4A45] 83€

R>99.5%@343 T>95%@515+1030 uvFSØ12.7x2mm 1-OS-2-0127-2-[4B00] 1-OS-2-0127-2-[4B45] 65€Ø25.4x5mm 1-OS-2-0254-5-[4B00] 1-OS-2-0254-5-[4B45] 71€

R>99.5%@355 T>95%@532+1064 BK7Ø12.7x3mm 1-OS-1-0127-3-[4C00] 1-OS-1-0127-3-[4C45] 55€Ø25.4x6mm 1-OS-1-0254-6-[4C00] 1-OS-1-0254-6-[4C45] 61€

R>99.5%@400 T>95%@800 uvFSØ12.7x2mm 1-OS-2-0127-2-[4D00] 1-OS-2-0127-2-[4D45] 61€Ø25.4x5mm 1-OS-2-0254-5-[4D00] 1-OS-2-0254-5-[4D45] 67€

R>99.5%@515 T>95%@1030 uvFSØ12.7x2mm 1-OS-2-0127-2-[4E00] 1-OS-2-0127-2-[4E45] 61€

Ø25.4x5mm 1-OS-2-0254-5-[4E00] 1-OS-2-0254-5-[4E45] 67€

R>99.5%@515T>90%@630-1300(AOI=0°),T>85%@630-1300(AOI=45°)

uvFSØ12.7x2mm 1-OS-2-0127-2-[4F00] 1-OS-2-0127-2-[4F45] 61€

Ø25.4x5mm 1-OS-2-0254-5-[4F00] 1-OS-2-0254-5-[4F45] 67€

R>99.5%@532 T>90%@266 uvFSØ12.7x2mm 1-OS-2-0127-2-[4G00] 1-OS-2-0127-2-[4G45] 61€Ø25.4x5mm 1-OS-2-0254-5-[4G00] 1-OS-2-0254-5-[4G45] 67€

R>99.5%@532 T>95%@1064 BK7Ø12.7x3mm 1-OS-1-0127-3-[4H00] 1-OS-1-0127-3-[4H45] 55€Ø25.4x6mm 1-OS-1-0254-6-[4H00] 1-OS-1-0254-6-[4H45] 61€

R>99.5%@(532+1064) T>90%@355 uvFSØ12.7x2mm 1-OS-2-0127-2-[4J00] 1-OS-2-0127-2-[4J45] 67€Ø25.4x5mm 1-OS-2-0254-5-[4J00] 1-OS-2-0254-5-[4J45] 73€

R>99.5%@(532+1064) T>95%@808 BK7Ø12.7x3mm 1-OS-1-0127-3-[4K00] 1-OS-1-0127-3-[4K45] 55€Ø25.4x6mm 1-OS-1-0254-6-[4K00] 1-OS-1-0254-6-[4K45] 61€

R>99.5%@(750-850) T>95%@532 uvFSØ12.7x2mm 1-OS-2-0127-2-[4L00] 1-OS-2-0127-2-[4L45] 61€Ø25.4x5mm 1-OS-2-0254-5-[4L00] 1-OS-2-0254-5-[4L45] 67€

R>99.5%@800 T>95%@400 uvFSØ12.7x2mm 1-OS-2-0127-2-[4M00] 1-OS-2-0127-2-[4M45] 61€Ø25.4x5mm 1-OS-2-0254-5-[4M00] 1-OS-2-0254-5-[4M45] 67€

R>99.5%@800 T>95%@1100-1600 uvFSØ12.7x2mm 1-OS-2-0127-2-[4n00] 1-OS-2-0127-2-[4n45] 65€Ø25.4x5mm 1-OS-2-0254-5-[4n00] 1-OS-2-0254-5-[4n45] 71€

R>99.5%@1030 T>95%@515 uvFSØ12.7x2mm 1-OS-2-0127-2-[4P00] 1-OS-2-0127-2-[4P45] 61€Ø25.4x5mm 1-OS-2-0254-5-[4P00] 1-OS-2-0254-5-[4P45] 67€

R>99.5%@1030 T>95%@940 BK7Ø12.7x3mm 1-OS-1-0127-3-[4R00] 1-OS-1-0127-3-[4R45] 79€Ø25.4x6mm 1-OS-1-0254-6-[4R00] 1-OS-1-0254-6-[4R45] 85€

R>99.5%@1020-1200 T>95%@970-980 uvFSØ12.7x2mm 1-OS-2-0127-2-[4S00] 1-OS-2-0127-2-[4S45] 225€Ø25.4x5mm 1-OS-2-0254-5-[4S00] 1-OS-2-0254-5-[4S45] 267€

R>99.5%@1064 T>95%@355 uvFSØ12.7x2mm 1-OS-2-0127-2-[4T00] 1-OS-2-0127-2-[4T45] 67€Ø25.4x5mm 1-OS-2-0254-5-[4T00] 1-OS-2-0254-5-[4T45] 73€

R>99.5%@1064 T>95%@532 BK7Ø12.7x3mm 1-OS-1-0127-3-[4v00] 1-OS-1-0127-3-[4v45] 55€Ø25.4x6mm 1-OS-1-0254-6-[4v00] 1-OS-1-0254-6-[4v45] 61€

R>99.5%@1064 T>95%@400-700 BK7Ø12.7x3mm 1-OS-1-0127-3-[4W00] 1-OS-1-0127-3-[4W45] 55€Ø25.4x6mm 1-OS-1-0254-6-[4W00] 1-OS-1-0254-6-[4W45] 61€

R>99.5%@1064 T>95%@808 BK7Ø12.7x3mm 1-OS-1-0127-3-[4X00] 1-OS-1-0127-3-[4X45] 55€Ø25.4x6mm 1-OS-1-0254-6-[4X00] 1-OS-1-0254-6-[4X45] 61€

CatalogItemsWavelength separators


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MeasuredreflectivityR>99.5%@0°,Rs>99.3%andRp>98.5%@45°


DuALLASERLInEREFLECTInGMIRRORS(DHR)

Dual laser line reflecting mirrors (DHR) provide optimizedreflection at two certain wavelengths at certain angle of incidence(AOI).Thesemultilayercoatingstackshelptoachievethe highest possible reflectivity at two specific laser line wavelengths at any designed angle of incidence. Laser line high reflectivity coatings are used in external beam manipulationapplications where losses are intolerable.

Description


Features

Miscellaneous

• Thecoatingsaredesignedtoachievethehighestpossiblereflectivity at two specific laser line wavelengths at normal or 45degreesincidence


• Massproductioncapabilities:10’000piecespermonth• Any other standard substrates can be coated with these

types of coatings


ThemeasuredtransmissioncurvefordualwavelengthDHRcoatingcode8J45


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•Opticalsubstrates(page18) •HRlaserlinemirrors(HR)(page52)

•Metalliccoatedoptics(page70)

Wavelength,nm

Substrate material

ProductIDforAOI=0°


Price*1-6pcs

ProductIDforAOI=0°


Price*1-6pcs

Ø12.7mm Ø25.4mm266+532 uvFS 1-OS-2-0127-2-[5A00] 1-OS-2-0127-2-[5A45] 83€ 1-OS-2-0254-5-[5A00] 1-OS-2-0254-5-[5A45] 89€343+1030 uvFS 1-OS-2-0127-2-[5B00] 1-OS-2-0127-2-[5B45] 83€ 1-OS-2-0254-5-[5B00] 1-OS-2-0254-5-[5B45] 89€355+532 uvFS 1-OS-2-0127-2-[5C00] 1-OS-2-0127-2-[5C45] 83€ 1-OS-2-0254-5-[5C00] 1-OS-2-0254-5-[5C45] 89€355+1064 uvFS 1-OS-2-0127-2-[5D00] 1-OS-2-0127-2-[5D45] 83€ 1-OS-2-0254-5-[5D00] 1-OS-2-0254-5-[5D45] 89€399+556 BK7 1-OS-1-0127-3-[5E00] 1-OS-1-0127-3-[5E45] 75€ 1-OS-1-0254-6-[5E00] 1-OS-1-0254-6-[5E45] 83€400+800 BK7 1-OS-1-0127-3-[5F00] 1-OS-1-0127-3-[5F45] 75€ 1-OS-1-0254-6-[5F00] 1-OS-1-0254-6-[5F45] 83€426+852 BK7 1-OS-1-0127-3-[5G00] 1-OS-1-0127-3-[5G45] 75€ 1-OS-1-0254-6-[5G00] 1-OS-1-0254-6-[5G45] 83€515+1030 BK7 1-OS-1-0127-3-[5H00] 1-OS-1-0127-3-[5H45] 75€ 1-OS-1-0254-6-[5H00] 1-OS-1-0254-6-[5H45] 83€532+1064 BK7 1-OS-1-0127-3-[5J00] 1-OS-1-0127-3-[5J45] 75€ 1-OS-1-0254-6-[5J00] 1-OS-1-0254-6-[5J45] 83€1064+1319 BK7 1-OS-1-0127-3-[5K00] 1-OS-1-0127-3-[5K45] 85€ 1-OS-1-0254-6-[5K00] 1-OS-1-0254-6-[5K45] 93€

CatalogItems

pLeASe noTe:thicknessofuvFSØ12.7mmis2mm;thicknessofBK7Ø12.7mmis3mmthicknessofuvFSØ25.4mmis5mm;thicknessofBK7Ø25.4mmis6mm•IfyoudonotfindsuitablewavelengthorAOIforyourapplicationpleasecontactusandwewillprovidethebestsolutionforyou!•Any of our standard substrates can be coated with these types of coatings•Curvedsubstratescanalsobecoated

Duallaserlinereflectingmirrors(DHR)

•5BM69T-1-kinematicopticalmountofsidedrive(page227)

•5BM131–beamsplitter/mirrormount(page220)


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Substrate wavefront distortion <λ/8




MeasuredresidualreflectivityR<0.2%@0°AOI,R<0.35%@45°AOI


ARCOATEDWInDOWS(AR)

Anti-reflectingcoatings(AR)aredesignedtoreducereflectivityof optical component to near-zero for a specific wavelength.

Description


Features

Miscellaneous

• Designedtoreducereflectivityofanopticalcomponenttonear-zero for a specific wavelength

• LaserlineAnti-Reflectioncoatingsinrange0,19um-10,6umare available


Relatedproductsandaccessories•Opticalsubstrates(page18)•4OCM-opticalcomponentmounts(page212)

•4H89–adjustableheightv-mount(page213)

MeasuredresidualbackreflectioncurveforARcoatingcode6P00


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BK7ARcoatedwindows

Wavelength, nm

ProductIDforAOI=0°

(residualreflectivity<0.2%)



Price*1-6pcs

ProductIDforAOI=0°




Price*1-6pcs

Ø12.7x3mm Ø25.4x6mm473-488 1-OS-1-0127-3-[6D00] 1-OS-1-0127-3-[6D45] 35€ 1-OS-1-0254-6-[6D00] 1-OS-1-0254-6-[6D45] 41€

515 1-OS-1-0127-3-[6E00] 1-OS-1-0127-3-[6E45] 35€ 1-OS-1-0254-6-[6E00] 1-OS-1-0254-6-[6E45] 41€527 - 532 1-OS-1-0127-3-[6F00] 1-OS-1-0127-3-[6F45] 35€ 1-OS-1-0254-6-[6F00] 1-OS-1-0254-6-[6F45] 41€

589 1-OS-1-0127-3-[6G00] 1-OS-1-0127-3-[6G45] 35€ 1-OS-1-0254-6-[6G00] 1-OS-1-0254-6-[6G45] 41€633 1-OS-1-0127-3-[6H00] 1-OS-1-0127-3-[6H45] 35€ 1-OS-1-0254-6-[6H00] 1-OS-1-0254-6-[6H45] 41€780 1-OS-1-0127-3-[6J00] 1-OS-1-0127-3-[6J45] 35€ 1-OS-1-0254-6-[6J00] 1-OS-1-0254-6-[6J45] 41€800 1-OS-1-0127-3-[6K00] 1-OS-1-0127-3-[6K45] 35€ 1-OS-1-0254-6-[6K00] 1-OS-1-0254-6-[6K45] 41€852 1-OS-1-0127-3-[6L00] 1-OS-1-0127-3-[6L45] 35€ 1-OS-1-0254-6-[6L00] 1-OS-1-0254-6-[6L45] 41€946 1-OS-1-0127-3-[6M00] 1-OS-1-0127-3-[6M45] 35€ 1-OS-1-0254-6-[6M00] 1-OS-1-0254-6-[6M45] 41€980 1-OS-1-0127-3-[6n00] 1-OS-1-0127-3-[6n45] 35€ 1-OS-1-0254-6-[6n00] 1-OS-1-0254-6-[6n45] 41€1030 1-OS-1-0127-3-[6P00] 1-OS-1-0127-3-[6P45] 35€ 1-OS-1-0254-6-[6P00] 1-OS-1-0254-6-[6P45] 41€

1047-1064 1-OS-1-0127-3-[6R00] 1-OS-1-0127-3-[6R45] 35€ 1-OS-1-0254-6-[6R00] 1-OS-1-0254-6-[6R45] 41€1122 1-OS-1-0127-3-[6S00] 1-OS-1-0127-3-[6S45] 35€ 1-OS-1-0254-6-[6S00] 1-OS-1-0254-6-[6S45] 41€1319 1-OS-1-0127-3-[6T00] 1-OS-1-0127-3-[6T45] 35€ 1-OS-1-0254-6-[6T00] 1-OS-1-0254-6-[6T45] 41€1550 1-OS-1-0127-3-[6v00] 1-OS-1-0127-3-[6v45 35€ 1-OS-1-0254-6-[6v00] 1-OS-1-0254-6-[6v45] 41€

uvFSARcoatedwindows

Wavelength, nm

ProductIDforAOI=0°




Price*1-6pcs

ProductIDforAOI=0°




Price*1-6pcs

Ø12.7x2mm Ø25.4x5mm266 1-OS-2-0127-2-[6A00] 1-OS-2-0127-2-[6A45] 43€ 1-OS-2-0254-5-[6A00] 1-OS-2-0254-5-[6A45] 49€

343-355 1-OS-2-0127-2-[6B00] 1-OS-2-0127-2-[6B45] 41€ 1-OS-2-0254-5-[6B00] 1-OS-2-0254-5-[6B45] 47€400 1-OS-2-0127-2-[6C00] 1-OS-2-0127-2-[6C45] 41€ 1-OS-2-0254-5-[6C00] 1-OS-2-0254-5-[6C45] 47€

473-488 1-OS-2-0127-2-[6D00] 1-OS-2-0127-2-[6D45] 41€ 1-OS-2-0254-5-[6D00] 1-OS-2-0254-5-[6D45] 47€515 1-OS-2-0127-2-[6E00] 1-OS-2-0127-2-[6E45] 41€ 1-OS-2-0254-5-[6E00] 1-OS-2-0254-5-[6E45] 47€

527 - 532 1-OS-2-0127-2-[6F00] 1-OS-2-0127-2-[6F45] 41€ 1-OS-2-0254-5-[6F00] 1-OS-2-0254-5-[6F45] 47€589 1-OS-2-0127-2-[6G00] 1-OS-2-0127-2-[6G45] 41€ 1-OS-2-0254-5-[6G00] 1-OS-2-0254-5-[6G45] 47€633 1-OS-2-0127-2-[6H00] 1-OS-2-0127-2-[6H45] 41€ 1-OS-2-0254-5-[6H00] 1-OS-2-0254-5-[6H45] 47€780 1-OS-2-0127-2-[6J00] 1-OS-2-0127-2-[6J45] 41€ 1-OS-2-0254-5-[6J00] 1-OS-2-0254-5-[6J45] 47€800 1-OS-2-0127-2-[6K00] 1-OS-2-0127-2-[6K45] 41€ 1-OS-2-0254-5-[6K00] 1-OS-2-0254-5-[6K45] 47€852 1-OS-2-0127-2-[6L00] 1-OS-2-0127-2-[6L45] 41€ 1-OS-2-0254-5-[6L00] 1-OS-2-0254-5-[6L45] 47€946 1-OS-2-0127-2-[6M00] 1-OS-2-0127-2-[6M45] 41€ 1-OS-2-0254-5-[6M00] 1-OS-2-0254-5-[6M45] 47€980 1-OS-2-0127-2-[6n00] 1-OS-2-0127-2-[6n45] 41€ 1-OS-2-0254-5-[6n00] 1-OS-2-0254-5-[6n45] 47€1030 1-OS-2-0127-2-[6P00] 1-OS-2-0127-2-[6P45] 41€ 1-OS-2-0254-5-[6P00] 1-OS-2-0254-5-[6P45] 47€

1047-1064 1-OS-2-0127-2-[6R00] 1-OS-2-0127-2-[6R45] 41€ 1-OS-2-0254-5-[6R00] 1-OS-2-0254-5-[6R45] 47€1122 1-OS-2-0127-2-[6S00] 1-OS-2-0127-2-[6S45] 41€ 1-OS-2-0254-5-[6S00] 1-OS-2-0254-5-[6S45] 47€1319 1-OS-2-0127-2-[6T00] 1-OS-2-0127-2-[6T45] 41€ 1-OS-2-0254-5-[6T00] 1-OS-2-0254-5-[6T45] 47€1550 1-OS-2-0127-2-[6v00] 1-OS-2-0127-2-[6v45] 41€ 1-OS-2-0254-5-[6v00] 1-OS-2-0254-5-[6v45] 47€

CatalogItems


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BROADBAnDARCOATEDWInDOWS(BBAR)

BroadbandARcoatingsaredesignedto reducethe reflectivityof optical component to near-zero for broad wavelength range.BroadbandARcoatingsworkingintherangeof190nmto10.6µm are available. These multilayer broadband anti-reflective coatings increasetransmissionofopticalelementforabroadspectrum.Therefore,it is ideal for a wide range of multi-wavelength laser and white light sources. The wavelength range and reflectivity of thecoating depends on the angle of incidence.

Description


Features

Miscellaneous

• Thesecoatingsaredesignedtoincreasetransmissionoverbroad spectrum


• BroadbandAnti-Reflectioncoatingsintherangeof0,19umto10,6umareavailable

MeasuredresidualbackreflectioncurveforBBARcoatingcode7C00


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• 4FH56-multiplefilterholder(page213)

• 5BM141-Mirroropticalmount(page220)

BK7ARcoatedwindows

Wavelength, nm

ResidualreflectivityAOI=0°,

%

ProductIDforAOI=0°


Price*1-6pcs

ProductIDforAOI=0°


Price*1-6pcs

Ø12.7x3mm Ø25.4x6mm

400-700 <1.0 1-OS-1-0127-3-[7A00] 1-OS-1-0127-3-[7A45] 48€ 1-OS-1-0254-6-[7A00] 1-OS-1-0254-6-[7A45] 56€

600-1050 <0.8 1-OS-1-0127-3-[7B00] 1-OS-1-0127-3-[7B45] 48€ 1-OS-1-0254-6-[7B00] 1-OS-1-0254-6-[7B45] 56€700-950 <0.4 1-OS-1-0127-3-[7C00] 1-OS-1-0127-3-[7C45] 48€ 1-OS-1-0254-6-[7C00] 1-OS-1-0254-6-[7C45] 56€750-850 <0.3 1-OS-1-0127-3-[7D00] 1-OS-1-0127-3-[7D45] 48€ 1-OS-1-0254-6-[7D00] 1-OS-1-0254-6-[7D45] 56€750-1000 <0.5 1-OS-1-0127-3-[7E00] 1-OS-1-0127-3-[7E45] 48€ 1-OS-1-0254-6-[7E00] 1-OS-1-0254-6-[7E45] 56€900-1200 <0.6 1-OS-1-0127-3-[7F00] 1-OS-1-0127-3-[7F45] 48€ 1-OS-1-0254-6-[7F00] 1-OS-1-0254-6-[7F45] 56€1200-1500 <0.6 1-OS-1-0127-3-[7G00] 1-OS-1-0127-3-[7G45] 48€ 1-OS-1-0254-6-[7G00] 1-OS-1-0254-6-[7G45] 56€1500-1900 <0.7 1-OS-1-0127-3-[7H00] 1-OS-1-0127-3-[7H45] 48€ 1-OS-1-0254-6-[7H00] 1-OS-1-0254-6-[7H45] 56€

CatalogItems

*[email protected]


• 4H89–adjustableheightv-mount(page213)

• Optical substrates (page18)


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Residualreflectivity <0.5%



DuALARCOATEDWInDOWS(DAR)

DualARcoatedwindowsaredesignedtoreducethereflectivityof optical component to near-zero for two wavelengths.

Usually these windows are used in multi-frequency laser output systems(e.g.frequencydoublers).

This type of coating provides very high transmission at twodifferent wavelengths.

Description


Features

Miscellaneous

• Thesecoatingsaredesignedtoincreasetransmissionoverabroad spectrum


• BroadbandAnti-Reflectioncoatingsintherangeof0,19umto10,6umareavailable

MeasuredresidualbackreflectioncurveforDARcoatingcode8J00


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• 4PH132-universalplateholder(page214)

• 4H29-pushholder(page213)

Wavelength, nm

Substrate material

ProductIDforAOI=0°


Price*1-6 pcs

ProductIDforAOI=0°


Price*1-6 pcs

Ø12.7x3mm Ø25.4x5mm

266+532 uvFS 1-OS-2-0127-2-[8A00] 1-OS-2-0127-2-[8A45] 47€ 1-OS-2-0254-5-[8A00] 1-OS-2-0254-5-[8A45] 53€

343+1030 uvFS 1-OS-2-0127-2-[8B00] 1-OS-2-0127-2-[8B45] 47€ 1-OS-2-0254-5-[8B00] 1-OS-2-0254-5-[8B45] 53€355+532 uvFS 1-OS-2-0127-2-[8C00] 1-OS-2-0127-2-[8C45] 47€ 1-OS-2-0254-5-[8C00] 1-OS-2-0254-5-[8C45] 53€355+1064 uvFS 1-OS-2-0127-2-[8D00] 1-OS-2-0127-2-[8D45] 47€ 1-OS-2-0254-5-[8D00] 1-OS-2-0254-5-[8D45] 53€399+556 BK7 1-OS-1-0127-3-[8E00] 1-OS-1-0127-3-[8E45] 41€ 1-OS-1-0254-6-[8E00] 1-OS-1-0254-6-[8E45] 47€400+800 BK7 1-OS-1-0127-3-[8F00] 1-OS-1-0127-3-[8F45] 41€ 1-OS-1-0254-6-[8F00] 1-OS-1-0254-6-[8F45] 47€426+852 BK7 1-OS-1-0127-3-[8G00] 1-OS-1-0127-3-[8G45] 41€ 1-OS-1-0254-6-[8G00] 1-OS-1-0254-6-[8G45] 47€515+1030 BK7 1-OS-1-0127-3-[8H00] 1-OS-1-0127-3-[8H45] 41€ 1-OS-1-0254-6-[8H00] 1-OS-1-0254-6-[8H45] 47€532+1064 BK7 1-OS-1-0127-3-[8J00] 1-OS-1-0127-3-[8J45] 41€ 1-OS-1-0254-6-[8J00] 1-OS-1-0254-6-[8J45] 47€1064+1319 BK7 1-OS-1-0127-3-[8K00] 1-OS-1-0127-3-[8K45] 41€ 1-OS-1-0254-6-[8K00] 1-OS-1-0254-6-[8K45] 47€

CatalogItemsDualARcoatedwindows(DAR)

*[email protected]


• Optical substrates (page18)

• 4OCM-opticalcomponentmounts(page212)


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Substrate material BK7,uvFSforuvenhancedmirrors


Surfacequality(aftercoating) 40-20Scratch&Dig

Surfaceflatness(aftercoating) λ/4

Clearaperture >90%ofDiameter

Laser damage threshold>0,3J/cm2for10nspulses@1064nm(forgoldandsilvercoatings)

METALLICCOATEDOPTICS

Metalliccoatingscanbeusedatanyangleofincidencebecausetheyhaveextremelybroadbandreflectance.

Weoffergold(Au),silver(Ag)andaluminum(Al)highreflectioncoatings formed by vacuum deposition. All metallic reflectors can be over-coated with dielectric film of MgF2 or SiO2 inorder to prevent oxidation of themetallic surface andprovideabrasion resistance.

Description


Features

Miscellaneous

• Protectedgoldprovidesexcellent,broadbandinfraredhighreflectance

• ProtectedsilverprovideshigherreflectancethanaluminumthroughoutthevisibleandnearIR

• ProtectedaluminumisaneconomicalsolutionforvISapplications

• uvenhancedaluminumprovidesgoodreflectanceoverawiderangeandismainlyusedinuvapplications

• Thesecoatingscanbedepositedonopticalsubstratesofvarious shapes and different curvatures

Typicalreflectivityofmetalcoatings


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• Opticalsubstrates(page18)• HRbroadbandmirrors(BBHR)(page54) • 5BM121T–beamsplitters/opticsmount(page222)

• 5OM10T–smallopticalmountofsidedrive(page226)

• 5OM122T–mirrormounts/tiltplatformsofsidedrive(page226)


CoatingtypeDimensions,

mmType ProductID

Price*1-9 pcs

uvenhancedAluminum

R>87%@250-350

Ø12,7x6 FLAT/FLAT 1-OS-2-0127-6-[9AL1] 30€Ø25,4x5 FLAT/FLAT 1-OS-2-0254-5-[9AL1] 34€

Ø25,4

Plano-Concave,ROC=-50mm 1-PCv-2-D254-[9AL1] 42€Plano-Concave,ROC=-100mm 1-PCv-2-F254-[9AL1] 42€Plano-Concave,ROC=-200mm 1-PCv-2-J254-[9AL1] 42€Plano-Concave,ROC=-500mm 1-PCv-2-L254-[9AL1] 42€Plano-Concave,ROC=-1000mm 1-PCv-2-M254-[9AL1] 42€


ProtectedAlumi-num

R>85%@350-IR


Ø25,4

Plano-Concave,ROC=-50mm 1-PCv-1-D254-[9AL0] 36€Plano-Concave,ROC=-100mm 1-PCv-1-F254-[9AL0] 36€Plano-Concave,ROC=-200mm 1-PCv-1-J254-[9AL0] 36€Plano-Concave,ROC=-500mm 1-PCv-1-L254-[9AL0] 36€Plano-Concave,ROC=-1000mm 1-PCv-1-M254-[9AL0] 36€


ProtectedSilverR>96%@400-IR

Ø12,7x6 FLAT/FLAT 1-OS-1-0127-6-[9AG0] 30€Ø25,4x6 FLAT/FLAT 1-OS-1-0254-6-[9AG0] 34€

Ø25,4

Plano-Concave,ROC=-50mm 1-PCv-1-D254-[9AG0] 42€Plano-Concave,ROC=-100mm 1-PCv-1-F254-[9AG0] 42€Plano-Concave,ROC=-200mm 1-PCv-1-J254-[9AG0] 42€Plano-Concave,ROC=-500mm 1-PCv-1-L254-[9AG0] 42€Plano-Concave,ROC=-1000mm 1-PCv-1-M254-[9AG0] 42€

Ø50,8x8 FLAT/FLAT 1-OS-1-0508-8-[9AG0] 74€Ø76,2x8 FLAT/FLAT 1-OS-1-0762-8-[9AG0] 100€

ProtectedGoldR>98%@900-IR

Ø12,7x6 FLAT/FLAT 1-OS-1-0127-6-[9Au0] 42€Ø25,4x6 FLAT/FLAT 1-OS-1-0254-6-[9Au0] 48€

Ø25,4

Plano-Concave,ROC=-50mm 1-PCv-1-D254-[9Au0] 56€Plano-Concave,ROC=-100mm 1-PCv-1-F254-[9Au0] 56€Plano-Concave,ROC=-200mm 1-PCv-1-J254-[9Au0] 56€Plano-Concave,ROC=-500mm 1-PCv-1-L254-[9Au0] 56€Plano-Concave,ROC=-1000mm 1-PCv-1-M254-[9Au0] 56€

Ø50,8x8 FLAT/FLAT 1-OS-1-0508-8-[9Au0] 90€Ø76,2x8 FLAT/FLAT 1-OS-1-0762-8-[9Au0] 140€

CatalogItems

*[email protected]



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Material Schott glass or equivalent


Clearaperture 90%


Surfaceflatness λ@632.8nm

Parallelism <3 arcmin

Uncoated, unmounted

COLORGLASSFILTERS

ALTECHnA provides color glass filters for laser pulse attenuation, filtering, etc.

Duetoitsselectiveabsorptioninthevisiblewavelengthrange,color glass filters will exhibit various colors depending on theglass type. Color glass filters provide economical solution forvariousapplications(filtering,attenuationetc.).

Optical glass filters are widely used in safety glasses, industrial measurement, environment protection and many other applications

Description


Features

Miscellaneous

• A color glass filter provides an economical solution for many various applications

• Foryourconvenience,wehaveselected45piecesofthecolor and neutral glass filters for various applications in the laboratory. Filters are assembled in a safe and compact woodenbox.youcandownloadfiltertransmissioncurvesforarangefrom200nmto1200nmfromourwebsite

• Customdesignproductionisalsoavailable• Checkthestockitemlistforfastestdelivery• Massproductioncapabilities:10’000piecespermonth


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MaterialProductID ProductID ProductIDØ12.7x3mm Ø25.4x3mm 50.8x50.8x3mm

GGSeries:yellowglassGG10 1-CF-GG10-0127 1-CF-GG10-0254 1-CF-GG10-5050GG375 1-CF-GG375-0127 1-CF-GG375-0254 1-CF-GG375-5050GG400 1-CF-GG400-0127 1-CF-GG400-0254 1-CF-GG400-5050GG420 1-CF-GG420-0127 1-CF-GG420-0254 1-CF-GG420-5050GG455 1-CF-GG455-0127 1-CF-GG455-0254 1-CF-GG455-5050GG475 1-CF-GG475-0127 1-CF-GG475-0254 1-CF-GG475-5050GG495 1-CF-GG495-0127 1-CF-GG495-0254 1-CF-GG495-5050

Price*1-5pcs 22€ 26€ 48€OGSeries:orangeglass

OG515 1-CF-OG515-0127 1-CF-OG515-0254 1-CF-OG515-5050OG530 1-CF-OG530-0127 1-CF-OG530-0254 1-CF-OG530-5050OG550 1-CF-OG550-0127 1-CF-OG550-0254 1-CF-OG550-5050OG570 1-CF-OG570-0127 1-CF-OG570-0254 1-CF-OG570-5050OG590 1-CF-OG590-0127 1-CF-OG590-0254 1-CF-OG590-5050

Price*1-5pcs 22€ 26€ 48€RGSeries:redandblackglass,IRtransmitting

RG6 1-CF-RG6-0127 1-CF-RG6-0254 1-CF-RG6-5050RG7 1-CF-RG7-0127 1-CF-RG7-0254 1-CF-RG7-5050RG610 1-CF-RG610-0127 1-CF-RG610-0254 1-CF-RG610-5050RG630 1-CF-RG630-0217 1-CF-RG630-0254 1-CF-RG630-5050RG645 1-CF-RG645-0127 1-CF-RG645-0254 1-CF-RG645-5050RG665 1-CF-RG665-0127 1-CF-RG665-0254 1-CF-RG665-5050RG695 1-CF-RG695-0127 1-CF-RG695-0254 1-CF-RG695-5050RG715 1-CF-RG715-0217 1-CF-RG715-0254 1-CF-RG715-5050RG780 1-CF-RG780-0127 1-CF-RG780-0254 1-CF-RG780-5050RG830 1-CF-RG830-0127 1-CF-RG830-0254 1-CF-RG830-5050RG850 1-CF-RG850-0127 1-CF-RG850-0254 1-CF-RG850-5050

Price*1-5pcs 22€ 26€ 48€uGSeries:blackblueglasses,ultraviolettransmitting

uG1 1-CF-uG1-0127 1-CF-uG1-0254 1-CF-uG1-5050uG5 1-CF-uG5-0127 1-CF-uG5-0254 1-CF-uG5-5050uG11 1-CF-uG11-0127 1-CF-uG11-0254 1-CF-uG11-5050

Price*1-5pcs 32€ 38€ 66€

KGSeries:colorlessglasswithhightransmissioninthevisibleandabsorptionintheIRrangeKG1 1-CF-KG1-0127 1-CF-KG1-0254 1-CF-KG1-5050KG2 1-CF-KG2-0127 1-CF-KG2-0254 1-CF-KG2-5050KG3 1-CF-KG3-0127 1-CF-KG3-0254 1-CF-KG3-5050

Price*1-5pcs 26€ 30€ 54€

CatalogItems


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vGSeries:greenglassvG5 1-CF-vG5-0127 1-CF-vG5-0254 1-CF-vG1-5050vG8 1-CF-vG8-0127 1-CF-vG8-0254 1-CF-vG8-5050vG10 1-CF-vG10-0127 1-CF-vG10-0254 1-CF-vG10-5050

Price*1-5pcs 22€ 26€ 48€BGSeries:blue,blue-greenandmulti-bandglass

BG3 1-CF-BG3-0127 1-CF-BG3-0254 1-CF-BG3-5050BG7 1-CF-BG7-0127 1-CF-BG7-0254 1-CF-BG7-5050BG12 1-CF-BG12-0127 1-CF-BG12-0254 1-CF-BG12-5050BG20 1-CF-BG20-0127 1-CF-BG20-0254 1-CF-BG20-5050BG25 1-CF-BG25-0127 1-CF-BG25-0254 1-CF-BG25-5050BG38 1-CF-BG38-0127 1-CF-BG38-0254 1-CF-BG38-5050

Price*1-5pcs 26€ 30€ 54€Colorandneutralfiltersetconsistingof45mountedfilters(Ø25.4mm,CA18mm)

universalFilterSet(45pcs) 1-uFS45-0254

Price 595€

CatalogItems

• Opticalsubstrates(page18)


• 5OM37-twoangularfineadjustmentmounts(page223)

• 4PH132-3-universalplateholder(page214)

• 4OFH-10-multiplefiltersholder(page214)



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Bandwidthtolerance ±20%maximal

Blocking <0.01%

Mountdiameter 25.4mm

Clearaperture >18mm

Temperaturelimits -50°Cto80°C

InTERFEREnCEFILTERS

ALTECHnA supplies high quality standard and custom-made interference filters operating within the spectral range from 250 nm to 5000 nm. We also offer biomedical band-pass filters, which are specially designed for biomedical in-strumentation including chemistry analysers and micro-plate readers. Fluorescence filters include such features as steep slopes, deep blocking (up to OD 6), minimal spectralcrosstalk, high transmission and environmental durability.

Description


Features

Miscellaneous

• Ingeneralinterferencefiltersareusedaswavelengthselectors in astrophysics, clinical chemistry, material analysis, quality control, and in general purpose laboratory colorimeters and other applications

•Customdesignproductionisavailable•Checkthestocklistitemsforfastestdelivery•Massproductioncapabilities:1’000piecespermonth


•5MBM24-mirrormounts(page224)


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Centralwavelength,

nm

Bandwidth(FWHM),nm

Peaktransmittance,%

ProductID

Price*1-5 pcs

uvbandpassfilters214 12 10 1-IF-0214 102€228 12 10 1-IF-0228 102€232 12 10 1-IF-0232 102€239 12 10 1-IF-0239 102€

254 12 12 1-IF-0254 102€

265 12 12 1-IF-0265 102€280 12 12 1-IF-0280 102€289 12 12 1-IF-0289 102€297 12 12 1-IF-0297 102€307 12 15 1-IF-0307 102€312 12 15 1-IF-0312 102€326 12 15 1-IF-0326 102€334 12 15 1-IF-0334 102€340 11 40 1-IF-0340 102€352 12 35 1-IF-0352 102€365 12 35 1-IF-0365 102€380 12 35 1-IF-0380 102€

vISnarrowbandpassfilters405 10 35 1-IF-0405 94€415 10 40 1-IF-0415 94€450 10 50 1-IF-0450 94€488 3 50 1-IF-0488 94€505 10 50 1-IF-0505 94€510 10 50 1-IF-0510 94€515 10 50 1-IF-0515 94€532 10 50 1-IF-0532 94€546 10 50 1-IF-0546 94€550 10 50 1-IF-0550 94€570 10 50 1-IF-0570 94€590 10 50 1-IF-0590 94€600 10 50 1-IF-0600 94€620 10 50 1-IF-0620 94€633 11 50 1-IF-0633 94€650 11 50 1-IF-0650 94€670 11 50 1-IF-0670 94€690 11 50 1-IF-0690 94€

CatalogItems

Centralwavelength,

nm

Bandwidth(FWHM),nm

Peaktransmittance,%

ProductID

Price*1-5 pcs

nIRnarrowbandpassfilters766 11 45 1-IF-0766 94€780 11 45 1-IF-0780 94€795 11 45 1-IF-0795 94€830 12 45 1-IF-0830 94€850 12 45 1-IF-0850 94€880 12 45 1-IF-0880 94€905 12 45 1-IF-0905 94€940 13 45 1-IF-0940 94€1060 10 45 1-IF-1060 94€1064 10 45 1-IF-1064 94€1152 11 45 1-IF-1152 94€1310 12 45 1-IF-1310 94€1320 12 45 1-IF-1320 94€1523 10 45 1-IF-1523 94€1550 10 45 1-IF-1550 94€

*[email protected]



•10WA168&10CWA168-variablewheelattenuators(page254)


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Material neutraldensityglass

DiameterTtlerance +0.00/-0.2mm

Clearaperture 90%


Surfaceflatness λ@632.8nm

Parallelismerror <3 arcmin

DesignedforvISrange(400-700nm)

Uncoated, unmounted

nEuTRALDEnSITyABSORPTIOnTyPEFILTERS

neutral density filters are ideal for overall light reduction incasesof extreme light intensity.neutral density laser radiationfilters with custom transmittance, dimensions and shapes are available. neutral density absorption type filters decreasethe intensity of light without altering the relative spectral distribution of the energy. Attenuation is accomplished by using an absorbing type of glass.

Description


Features

Miscellaneous

• neutraldensityfilterisaneconomicalsolutiontoattenuatelight.

•Customdesignproductionisalsoavailable•Checkthestocklistitemsforfastestdelivery•Massproductioncapabilities:1’000piecespermonth


• Opticalsubstrates(page18)• Opticalcoatings(pages86-98)




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OpticalDensity AverageTransmissioninvISProductID

Ø12.7mm Ø25.4mm 50.8x50.8mm

0.1 80% 1-nF-01-0127 1-nF-01-0254 1-nF-01-50500.2 60% 1-nF-02-0127 1-nF-02-0254 1-nF-02-50500.3 50% 1-nF-03-0127 1-nF-03-0254 1-nF-03-50500.4 40% 1-nF-04-0127 1-nF-04-0254 1-nF-04-50500.5 30% 1-nF-05-0127 1-nF-05-0254 1-nF-05-50500.8 15% 1-nF-08-0127 1-nF-08-0254 1-nF-08-50501.0 10% 1-nF-10-0127 1-nF-10-0254 1-nF-10-50501.5 3% 1-nF-15-0127 1-nF-15-0254 1-nF-15-50502.0 1% 1-nF-20-0127 1-nF-20-0254 1-nF-20-50503.0 0.1% 1-nF-30-0127 1-nF-30-0254 1-nF-30-5050Price

*1-5 pcs28€ 32€ 44€

Colorandneutraldensityfiltersetconsistingof45mountedfilters(Ø25.4mm,CA18mm)universalfilterset(45pcs) 1-uFS45-0254

Price 595€neutraldensityfiltersetconsistingof11mountedfilters(Ø25.4mm,CA18mm)

neutraldensityfilterset(11pcs) 1-nFS11-0254Price 198€

CatalogItems

*[email protected]



•8MRu-1-universalmotorizedrotationstage(page247)


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MaterialB-270opticalCrown;uvgradeFusedSilica

Outside diameter 25mm;50mm;100mm

Insidediameter 8.0mm

Designwavelength 400-700nm

Operating wavelength range380-2000nm(B-270);250-2500nm(uvgradeFusedSilica)

Coatedarea 0to270°

Parallelismerror ±3arcmin

CIRCuLARvARIABLEnEuTRALDEnSITyFILTERS

Standard Specifications

Features

Miscellaneous

• Circularvariableneutraldensityfilteriseconomicalsolutionto attenuate light.

•Customdesignproductionisavailable•Checkthestocklistitemsforfastestdelivery•Massproductioncapabilities:1’000piecespermonth

Circular nD filters provide continuously variable, linearattenuation of light by rotating the filter around its center. Transmitted intensityvariesasa functionoftheopticaldensityrange.Thefiltercanbeusedforwhitelightaswellasforlasers.Sizesareavailablefrom25mmtoover100mmindiameter.

Description


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Optical density range

Average transmission invIS

Substrate material Operating rangeProductID

Ø25mm Ø50mm Ø100mm

0.04to1.0 90%to10% B-270opticalcrown 380-2000nm 1-CnF-1-A025 1-CnF-1-A050 1-CnF-1-A100

Price*1-5 pcs

89€ 131€ 186€

0.04to2.0 90%to1% B-270opticalcrown 380-2000nm 1-CnF-2-A025 1-CnF-2-A050 1-CnF-2-A100

Price*1-5 pcs

89€ 131€ 186€

0.04to3.0 90%to0,1% B-270opticalcrown 380-2000nm 1-CnF-3-A025 1-CnF-3-A050 1-CnF-3-A100

Price*1-5 pcs

94€ 141€ 203€

0.04to1.0 90%to10% uvgradefusedsilica 250-2500nm 1-CnF-1-B025 1-CnF-1-B050 1-CnF-1-B100

Price*1-5 pcs

99€ 146€ 233€

0.04to2.0 90%to1% uvgradefusedsilica 250-2500nm 1-CnF-2-B025 1-CnF-2-B050 1-CnF-2-B100

Price*1-5 pcs

99€ 146€ 233€

0.04to3.0 90%to0,1% uvgradefusedsilica 250-2500nm 1-CnF-3-B025 1-CnF-3-B050 1-CnF-3-B100

Price*1-5 pcs

102€ 151€ 238€

CatalogItems


•5TOM2-1-twoaxistranslationopticalmount(page229)


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Material Aluminium



Surfacefigure 1/4λ-1λRMS(dependsonsize)

Surface roughness <100-175ÅRMS

Coating Protectedaluminumorprotectedgold

METALMIRRORS


Features

Miscellaneous

• Aluminum substrate mirrors •Availablein30°,60°,or90°Off-Axis•Mountingplatesalsoavailable

•Customdesignproductionisalsoavailable•Massproductioncapabilities:500piecespermonth•Checkthestocklistitemsforfastestdelivery

Standard and special metal mirrors with parabolic surface contours offer off-axis beam focusing performance. Thesemirrors are machined from solid bar stock to minimize surface figure deformation which is inherent to the thin walled replicatedtype.Themetalmirrorsareproducedwithadvanceddiamond turning equipment.

Description


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Diameter,mmParentfocallength, mm

Reflectedeffective FL, mm

Angle,°yoffsetaxis(mm)

Coating ProductIDPrice

*1-5 pcs50.8 50.8 54.45 30 27.22 Protectedgold 1-OPM-A508-[9Au0] 490€25.4 38.1 50.8 60 43.99 Protectedgold 1-OPM-A254-[9Au0] 320€25.4 12.7 25.4 90 25.4 Protectedgold 1-OPM-B254-[9Au0] 320€50.8 25.4 50.8 90 50.8 Protectedgold 1-OPM-B508-[9Au0] 480€25.4 50.8 101.6 90 101.6 Protectedgold 1-OPM-C254-[9Au0] 320€25.4 76.2 152.4 90 152.4 Protectedgold 1-OPM-D254-[9Au0] 320€50.8 76.2 152.4 90 152.4 Protectedgold 1-OPM-C508-[9Au0] 480€25.4 101.6 203.2 90 203.2 Protectedgold 1-OPM-E254-[9Au0] 320€

25.4 25.4 27.22 30 13.61 Protectedaluminum 1-OPM-F254-[9AL0] 310€25.4 50.8 54.45 30 27.22 Protectedaluminum 1-OPM-H254-[9AL0] 215€50.8 50.8 54.45 30 27.22 Protectedaluminum 1-OPM-A508-[9AL0] 385€50.8 101.6 108.89 30 54.45 Protectedaluminum 1-OPM-D508-[9AL0] 385€25.4 25.4 33.85 60 29.33 Protectedaluminum 1-OPM-J254-[9AL0] 225€25.4 38.1 50.8 60 43.99 Protectedaluminum 1-OPM-A254-[9AL0] 205€25.4 50.8 67.74 60 58.64 Protectedaluminum 1-OPM-K254-[9AL0] 205€50.8 76.2 101.6 60 87.98 Protectedaluminum 1-OPM-E508-[9AL0] 395€25.4 12.7 25.40 90 25.4 Protectedaluminum 1-OPM-B254-[9AL0] 205€25.4 25.4 50.80 90 50.8 Protectedaluminum 1-OPM-L254-[9AL0] 205€25.4 50.8 101.6 90 101.6 Protectedaluminum 1-OPM-C254-[9AL0] 205€25.4 101.6 203.2 90 203.2 Protectedaluminum 1-OPM-E254-[9AL0] 205€50.8 25.4 50.8 90 50.8 Protectedaluminum 1-OPM-B508-[9AL0] 375€50.8 50.8 101.60 90 101.6 Protectedaluminum 1-OPM-F508-[9AL0] 375€50.8 95.3 190.5 90 190.5 Protectedaluminum 1-OPM-G508-[9AL0] 375€

CatalogItems


•5F21-1-flippingmirror/beamsplittermount(page217)


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Material uvFS,BK7

Types Plano/Plano,PCv,PCX


Thicknesstolerance +/-0.1mm

Flatness λ/10


Paralellismerror(PL/PL) <10arcsec

Clearaperture >90%

Coatingdamagethreshold >10J/cm2for10nspulses@1064nm

vARIABLEREFLECTIvITyMIRRORS


Features

Miscellaneous

•Improvesbeamshapeandquality•variable/locallydefinedreflection•HighestavailablecentralreflectionvalueR

r(max)–50%

•Customdesign(substrateshape,wedge,ARcoating)available

•Customdesignproductionisalsoavailable•Massproductioncapabilities:500piecespermonth•Checkthestockitemslistforfastestdelivery

Inordertohavebetterbeamquality,i.e.innon-stableresonators,variable reflection mirrors can be used. High intensity of thelaser beam requires use of components with a high damage threshold. Dielectric coatings are best suited to meet theserequirements. ALTECHnA offers variable reflectivity mirrors with dielectric coatings, designed for wavelengths in the range from 266to2500nm.

Function of reflection. Expression:r - radius (variable), mmRr - Reflection (mean), %R0 - Reflection (center), %wm - coating 1/e-radius, mmk - order

Description


• Optical positioners •Opticalcoatings(pages86-98)


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Material BK7gradeA,opticalglass

Dimensiontolerance ±0.1mm


Surface quality 40-20ScratchesandDig

Angle tolerance ±2arcmin

Clearaperture >85%

Bevel 0.3mmx45°

Coatingtype Hybrid

Absorption <10%

(Rs-R

p) <5%

nOn-POLARIZInGBEAMSPLITTERCuBES

non-polarizing beamsplitter cubes are constructed bycementing two precision right angle prisms together with metallic-dielectric coating on the hypotenuse surface. Absorption loss due to coating is around 10%. Due to coatingdesign, these cubes do not affect the polarization of the beam.

Description


Features

• All faces are Anti-reflection coated• Low polarization dependence

Miscellaneous

• Customdesignproductionisalsoavailable• Other sizes, split ratios and wavelengths are available

upon request• non-polarizingbeamsplittercubeswithpurelydielectric

coatings are available

Typicalperformanceof1-nC-2-1250element


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• 6PT169-threeangleprism/beamsplittertable(page232)

• 5MO111-mirror/opticsmount

RelatedproductsandaccessoriesBeamsplittingRatio

Dimensions,mmWavelength,

nmProductID

Price*1-5 pcs

Tp=T

s=45±5%;

Rp=R

s=45±5%

5x5x5

450-680 1-nC-1-0550 105€532 1-nC-2-0550 95€

700-1000 1-nC-3-0550 105€1064 1-nC-4-0550 95€

900-1200 1-nC-5-0550 105€

12.7x12.7x12.7

450-680 1-nC-1-1250 120€532 1-nC-2-1250 105€

700-1000 1-nC-3-1250 120€1064 1-nC-4-1250 105€

900-1200 1-nC-5-1250 120€

20x20x20

450-680 1-nC-1-2050 130€532 1-nC-2-2050 110€

700-1000 1-nC-3-2050 130€1064 1-nC-4-2050 110€

900-1200 1-nC-5-2050 130€

CatalogItems

*[email protected]



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DIELECTRICCOATInGS

Dielectric coatings consist of layers with different refractiveindices. There are three major techniques used for dielectriccoating: electron-beam deposition (E-beam), ion-assistedelectron-beam (IAD) and ion beam sputtering (IBS). All oftheseprocessesarequitesimilar intheirprinciple.Theyconsistof evaporating some coating material and deposit it on the substrate.Thedifferenceliesinthedepositionenergy.

Because of low energies involved when using electron-beamdeposition, thin film contains bubbles and micropores like a sponge.Thesewilleventually fillwithwater,whichwillchangethe refractive index of the coating and thus the propertiesof the optics. ( This is known as “environmental shifting”). Thepresence of water also lowers the damage threshold of the optics:whenexposedtoanintenselight,thewaterwilltendtovaporise and dislodge off bits of the coating. Finally, even in the absence of water, inhomogeneities of coating layers decrease the theoretical damage threshold. The positive points aboutthis technology is that it is cost effective, widespread and very versatile.Thecoatingitself isalsoslightlyflexible,whichmakesthe optics more resistant to mechanical stress.

Ion-assisted electron-beam is an intermediate technique,betweenion-beamsputteringandE-beam.Soareitsresults.

Ion beam sputtering involves energies 100 times higher than

Description

E-beams. As a result themolecules of the coating layers formcovalent bound when deposited. The resulting coating is freefrom bubbles or pores, more homogeneous, more durable, has higher damage threshold and is more repeatable and controllable. It also exhibits lower scattering and absorptionproperties, and overall higher specifications (more broadband, steeper transitions when needed, better spectral stability…).Thisishighprecisioncoating,andthesurfaceroughnesscanbecontrolledatbetterthan1ÅRMS(!),thatis<λ/5000.Ofcourse,this comes at a higher cost (atom-by-atom removal is very slow),andevenworse,itislimitedinthetypesofcoatingsitcanhandle:most of the uv coatings for instance involve fluorideswhich dissociate when sputtered. In this case, E-beam is theonly option.


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MeasuredreflectivityR>99,5%@0°;Rs>99,8%andRp>99,3%@45°


HRLASERLInECOATInGS(HR)


Features

Miscellaneous

• Provideanoptimizedperformanceatcertainwavelengthandcertainangleofincidence(AOI)


• HRlaserlinecoatings(HR)highlyreflectwavelengthrangeof<10%ofthecentralwavelength(CWL).Forinstance,HR@800nmwillreflectwavelengthrangeof760-840nm

• Ifyourapplicationneedstoreflectawiderwavelengthrangepleasereferto-broadbandHRwavelength(BBHR)coatings

HR laser line mirrors (HR) provide optimized performance atcertainwavelengthandcertainangleof incidence(AOI).Mirrorconsists of substrate and multilayer coating stacks which help to achieve very high reflectivity at specific laser line wavelength at anydesignedangleofincidence.LaserlineHRcoatingsareusedforexternalbeammanipulationapplicationswhereevenslightlossesmay be intolerable. Coatings are provided by Ion BeamSputtering(IBS)orelectronbeamevaporationwith/withoutionassistance coating techniques.


Description Measuredtransmissioncurveofthestandardcoatingcode1E45


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Wavelength, nmReflectivity(average),%

CoatingcodeforAOI=0°


266 >99.0 1A00 1A45343-355 >99.5 1B00 1B45

400 >99.5 1C00 1C45473-488 >99.5 1D00 1D45

515 >99.5 1E00 1E45527 - 532 >99.5 1F00 1F45

589 >99.5 1G00 1G45633 >99.5 1H00 1H45780 >99.5 1J00 1J45800 >99.5 1K00 1K45852 >99.5 1L00 1L45946 >99.5 1M00 1M45980 >99.5 1n00 1n451030 >99.5 1P00 1P45

1047-1064 >99.5 1R00 1R451122 >99.5 1S00 1S451319 >99.5 1T00 1T451550 >99.5 1v00 1v45

CatalogItems



• HRlaserlinemirrors(HR)(page52)

• HRbroadbandmirrors(BBHR)(page54)

*[email protected]

Ifyoudonotfindsuitableparametersor need other wavelengths design for your application please contact us and we guaranty to provide a solution for you


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Measuredreflectivity R>99%@0°;Rave>99%@45°


HRBROADBAnDCOATInGS(BBHR)

HR broad band mirrors (BBHR) provide high reflectivity for abroad spectrum.Therefore, it is ideal solution for awide rangeofmulti-wavelength laser orwhite light applications. Coatingsare provided by Ion Beam Sputtering (IBS) or electron beamevaporation with/without ion assistance coating techniques.


Description


Features

Miscellaneous

• Provideanoptimizedperformanceoverabroadwavelengthrange


CatalogItems


Reflectivity(average),%

coating code forAOI=0°

coating code for AOI=45°

400-700 >99.0 2A00 2A45700-950 >99.0 2B00 2B45750-850 >99.0 2C00 2C45750-1000 >99.0 2D00 2D45900-1200 >99.0 2E00 2E45

Measuredtransmissioncurveofthestandardcoatingcode2C00



• HRlaserlinemirrors(HR)(page52)• HRbroadbandmirrors(BBHR)(page54)


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PARTIALREFLECTInGCOATInGS(PR)

Partial reflecting coatings (PR) provide required percentagereflection/transmission at a specific angle of incidence for both single and broad band wavelengths. These coatings usuallyserve for efficient beam splitting as well as output coupling in high power laser cavities.

Description


Features

Miscellaneous

• Efficientbeamsplittingaswellasoutputcouplinginhighpower laser cavities


MeasuredtransmissioncurveforPRcoatingcode3F00-50




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Wavelength, nm Reflectivity(s-pol),%Coatingcodefor

AOI=0°Coatingcodefor

AOI=45°

26610±3 3A00-10 3A45-1050±2 3A00-50 3A45-5090±1 3A00-90 3A45-90

35510±3 3B00-10 3B45-1050±2 3B00-50 3B45-5090±1 3B00-90 3B45-90

40010±3 3C00-10 3C45-1050±2 3C00-50 3C45-5090±1 3C00-90 3C45-90

515 - 53210±3 3D00-10 3D45-1050±2 3D00-50 3D45-5090±1 3D00-90 3D45-90

63310±3 3E00-10 3E45-1050±2 3E00-50 3E45-5090±1 3E00-90 3E45-90

750-85010±3 3F00-10 3F45-1050±2 3F00-50 3F45-5090±1 3F00-90 3F45-90

94610±3 3G00-10 3G45-1050±2 3G00-50 3G45-5090±1 3G00-90 3G45-90

1020-110010±3 3H00-10 3H45-1050±2 3H00-50 3H45-5090±1 3H00-90 3H45-90

112210±3 3J00-10 3J45-1050±2 3J00-50 3J45-5090±1 3J00-90 3J45-90

131910±3 3K00-10 3K45-1050±2 3K00-50 3K45-5090±1 3K00-90 3K45-90

155010±3 3L00-10 3L45-1050±2 3L00-50 3L45-5090±1 3L00-90 3K45-90

CatalogItems


• Partialreflectingmirrors(page54)

• nonpolarizingbeamsplittercubes(page84)

*[email protected]



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WAvELEnGTHSEPARATInGCOATInGS

Wavelength separating coatings are used to separate the spectral regions or specified wavelengths (e.g. harmonic components)of multi-frequency laser systems by selective spectral reflection, transmission and absorption.

In all cases one wavelength is reflected while the others aretransmitted.

Description


Features

Miscellaneous

• Used to separate the spectral regions or specified wavelengths


Measuredtransmissioncurveforwavelengthseparatorcoatingcode4D45

*[email protected]



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Reflectedwavelength,nm Transmittedwavelength,nmCoatingcodeforAOI=0°


R>99%@266 T>90%@355+532+1064 4A00 4A45

R>99.5%@343 T>95%@515+1030 4B00 4B45R>99.5%@355 T>95%@532+1064 4C00 4C45R>99.5%@400 T>95%@800 4D00 4D45R>99.5%@515 T>95%@1030 4E00 4E45

R>99.5%@515T>85%@630-1300(AOI=0°),T>90%@630-1300(AOI=45°)

4F00 4F45

R>99.5%@532 T>90%@266 4G00 4G45R>99.5%@532 T>95%@1064 4H00 4H45

R>99.5%@(532+1064) T>90%@355 4J00 4J45R>99.5%@(532+1064) T>95%@808 4K00 4K45R>99.5%@(750-850) T>95%@532 4L00 4L45

R>99.5%@800 T>95%@400 4M00 4M45R>99.5%@800 T>95%@1100-1600 4n00 4n45R>99.5%@1030 T>95%@515 4P00 4P45R>99.5%@1030 T>95%@940 4R00 4R45R>99.5%@1030 T>95%@976 4S00 4S45R>99.5%@1064 T>95%@355 4T00 4T45R>99.5%@1064 T>95%@532 4v00 4v45R>99.5%@1064 T>95%@400-700 4W00 4W45R>99.5%@1064 T>95%@808 4X00 4X45

CatalogItems


• Opticalsubstrates(page18) • Wavelengthseparators(page60)


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MeasuredreflectivityR>99,5%@0°Rs>99,3%andRp>98,5%@45°


DuALLASERLInEREFLECTInGCOATInGS(DHR)

Dual laser line reflecting mirrors (DHR) provide optimizedreflection at two certain wavelengths at certain angle of incidence(AOI).These multilayer coating stacks help to achieve the highestpossible reflectivity at two specific laser line wavelengths at any designed angle of incidence. Laser line high reflectivity coatings are used in external beam manipulation applications wherelosses are intolerable.

Description


Features

Miscellaneous

• Thesecoatingsaredesignedtoachievethehighestpossiblereflectivity at two specific laser line wavelengths at normal or 45degreesincidence




• Metalliccoatedoptics(page70)

• Duallaserlinemirrors(page62)

MeasuredtransmissioncurvefordualwavelengthHRcoatingcode8J45

CatalogItems

Wavelength, nmReflectivityat

normalIncidence,%

Coatingcodefor

AOI=0°

Coatingcodefor

AOI=45°266+532 >99.0 5A00 5A45343+1030 >99.5 5B00 5B45355+532 >99.5 5C00 5C45355+1064 >99.5 5D00 5D45399+556 >99.5 5E00 5E45400+800 >99.5 5F00 5F45426+852 >99.5 5G00 5G45515+1030 >99.5 5H00 5H45532+1064 >99.5 5J00 5J451064+1319 >99.5 5K00 5K45


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MeasuredresidualreflectivityR<0.2%@0°AOI,R<0.4%@45°AOI


LASERLInEARCOATInGS(AR)

AR coatings are designed to reduce the reflectivity of acomponent to near-zero for a specific wavelength.

We supply standard laser line Anti-Reflection coatings in therange0,19um-10,6um.

Description


CatalogItems

Wavelength, nmResidualreflectivity,

%



266 <0.5 6A00 6A45343-355 <0.25 6B00 6B45

400 <0.2 6C00 6C45473-488 <0.2 6D00 6D45

515 <0.2 6E00 6E45527 - 532 <0.2 6F00 6F45

589 <0.2 6G00 6G45633 <0.2 6H00 6H45780 <0.2 6J00 6J45800 <0.2 6K00 6K45852 <0.2 6L00 6L45946 <0.2 6M00 6M45980 <0.2 6n00 6n451030 <0.2 6P00 6P45

1047-1064 <0.2 6R00 6R451122 <0.2 6S00 6S451319 <0.2 6T00 6T451550 <0.2 6v00 6v45

Relatedproductsandaccessories• Opticalsubstrates(page18)• ARcoatedwindows(page64)

MeasuredresidualbackreflectioncurveforARcoatingcode6P00

Miscellaneous


• LaserlineAnti-Reflectioncoatingsintherange0,19um-10,6um are available


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BROADBAnDARCOATInGS(BBAR)

BroadbandARcoatingsaredesignedto reducethe reflectivityof optical component to near-zero for broad wavelength range.BroadbandARcoatingsworkingintherangeof190nmto10.6µm are available. These multilayer broadband anti-reflectivecoatings increase transmission of optical element for a broad spectrum. Therefore, it is ideal for a wide range of multi-wavelength laser and white light sources. The wavelengthrange and reflectivity of the coating depends on the angle of incidence.

Description


Features

Miscellaneous

• Thesecoatingsaredesignedtoincreasethetransmissionovera broad spectrum


• BroadbandAnti-Reflectioncoatingsintherange0,19um-10,6umareavailable



• BroadbandARcoatedwindows(BBAR)(page66)

CatalogItems


Residualaveragereflectivity

AOI=0°,%



400-700 <1.0 7A00 7A45600-1050 <0.8 7B00 7B45700-950 <0.4 7C00 7C45750-850 <0.3 7D00 7D45750-1000 <0.5 7E00 7E45900-1200 <0.6 7F00 7F451200-1500 <0.6 7G00 7G451500-1900 <0.7 7H00 7H45266-370 <0.5 7J00 7J45

MeasuredresidualbackreflectioncurveforBBARcoatingcode7D00


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DuALARCOATInGS(DAR)

Dual AR coatings are designed to reduce the reflectivity of acomponent to near-zero for two certain wavelengths. Usually these coatings are used in multi-frequency laser output systems (e.g.frequencydoubling).

This type of coating provides very high transmission at twodifferent wavelengths. Typical wavelengths and reflectioncurvesof anARcoating suitable for theprevalent laser systemoutputat1064nmand532nmareshownbelow.

Description


CatalogItems

Wavelength, nm

Residualaveragereflectivity

AOI=0°,%



266+532 <0.5 8A00 8A45343+1030 <0.3 8B00 8B45355+532 <0.3 8C00 8C45355+1064 <0.3 8D00 8D45399+556 <0.3 8E00 8E45400+800 <0.3 8F00 8F45426+852 <0.3 8G00 8G45515+1030 <0.25 8H00 8H45532+1064 <0.25 8J00 8J451064+1319 <0.3 8K00 8K45



*ContactALTECHnAotherwavelengthsdesignforyourapplicationinfo@altechna.com

Miscellaneous


ThemeasuredresidualbackreflectioncurveforDARcoatingcode8J00

Features

• Frequently used in multi-frequency laser output systems (e.g. frequencydoubling)


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Laser damage threshold>0,3J/cm2for10nspulses@1064nm(forgoldandsilver)

METALLICCOATInGS

Metallic coatings are convenient in that they are extremelybroadband and can be used at any angle of incidence. Weoffergold(Au),silver(Ag)andaluminum(Al)highreflectioncoatings formed by vacuum deposition. All metallic reflectors can be over-coated with dielectric film of MgF2 or SiO2 inorder to prevent oxidation of themetallic surface andprovideabrasion resistance.

Description


Features

Miscellaneous

• Protectedgoldprovidesexcellent,broadbandinfraredhighreflectance

• ProtectedsilverprovideshigherreflectancethanaluminumthroughoutthevisibleandnearIR

• ProtectedaluminumiseconomicalsolutionforvISapplications

• uvenhancedaluminumprovidesgoodreflectanceoverawiderangeandaremainlyusedinuvapplications

• Thesecoatingscanbedoneonopticalsubstratesofvariousshape and curvature



• Metalliccoatedoptics(page70)

CatalogItems

Coatingtype Reflectivity,% Coatingcodeuvenhancedaluminum >83%@250-IR 9AL1Protectedaluminum >85%@350-IR 9AL0

Protectedsilver >96%@400-IR 9AG0Protectedgold >98%@900-IR 9Au0

*PleaserefertotheOpticalSubstratessectiontofindsuitable substrate for the metal coated mirrors


POLARIZATION OPTICS

WAVEPLATES (PHASE RETARDATION PLATES) 100

•Crystalline quartz waveplates 101

•High power waveplates 103

•Achromatic (broadband) waveplates 105

•Mid-IR Waveplates 107

SPECIAL OPTICS S-WAVEPLATE 108

BREWSTER TYPE THIN FILM POLARIZERS 109

BROADBAND (ULTRAFAST) THIN FILM POLARIZERS

111

POLARIZING CUBES 113

GLAN AND OTHER TYPE POLARIZERS 115

•High power laser Glan polarizers 115

•Glan Taylor polarizers 117

•Glan Thompson polarizers 119

•Wollaston polarizers 120

•Beamdisplacers 122

•Rochon polarizers 123


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WAVEPLATES (PHASE RETARDATION PLATES)BRIEF OVERVIEW

ALTECHNA is offering a wide range of zero order (ZO), low order (LO) half (L/2) or quarter (L/4) waveplates for UV, VIS, NIR and IR (for any wavelength in 240-9000 nm range).

Waveplates are made from materials which exhibit birefringence. The velocity of the extraordinary and ordinary rays through the birefringent material varies inversely with their refractive indi-ces. This difference in velocities gives a rise to phase difference. At any specific wavelength the phase difference is governed by the thickness of the retarder - waveplate.

Half (λ/2) waveplate. A linearly polarized beam incident on a half wave crystal quartz waveplate emerges as a linearly polar-ized beam but rotated such that its angle to the optical axis is twice that of the incident beam. Therefore, half-waveplates can be used as continuously adjustable polarization rotators. Half-waveplates are used to rotate the plane of polarization, electro-optic modulation and as a variable ratio beamsplitter when used in conjunction with a polarization cube.

Quarter (λ/4) waveplate - thin-film compensator. If the angle be-tween the electric field vector of the incident linearly polarized beam and the retarder principal plane of the quarter-waveplate is 45deg, the emergent beam is circularly polarized. When a quarter waveplate is double passed, i.e. by mirror reflection, it acts as a half waveplates and rotates the plane of polarization to a certain angle. Quarter waveplate are used in creating circular polarization from linear or linear polarization from circular, el-lipsometry, optical pumping, suppressing unwanted reflection and optical isolation.

Features

• Waveplates for any wavelength in the 240-9000 nm range• Air-spaced ZO waveplates for high energy applications• Waveplates for many wavelengths are available from stock• Custom design waveplate assemblies are available on request

Miscellaneous

• Zero order (ZO) waveplates are generally preferred since they are least sensitive to variations in wavelength, angle of incidence and temperature. To suit different applications, air spaced or optically contacted (see drawings on next page) Zero order compensated phase retardation plates are available from ALTECHNA

• The air-spaced construction enables to use the waveplate for high power laser applications. The damage threshold is more than 500 MW/cm2

Performance of half (λ/2) waveplate

Performance of quarter (λ/4) waveplate


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CRYSTALLINE QUARTZ WAVEPLATES

Description

Altechna is offering a wide range of zero order (ZO), low order (LO) waveplates for UV, VIS, NIR range (for any wavelength in 240-2600 nm range). All our waveplates are made from excellent quality laser grade crystalline quartz material.

ZO waveplate is constructed by two quartz plates with their fast axes crossed. The difference in thickness between the two plates determines the retardance. ZO waveplates offer a substantial-ly lower dependence on temperature, angle and wavelength change than conventional monolithic LO waveplates.

To suit different applications, air-spaced or optically contacted ZO compensated phase retardation waveplates are available from Altechna.

The air-spaced construction enables to use the waveplate for high power laser applications. The damage threshold is more than 500 MW/cm2.

ZO air-spaced ZO optically contacted LO waveplate

Low wavelength dependence Good for single wavelength use

Low temperature dependence Sensitive to temperature changes

More expensive than LO waveplates Cost effective

Retardation vs. wavelength for ZO and LO crystalline quartz waveplates


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ZO crystalline quartz waveplates (airspaced, mounted in 25.4 mm metal mount)

Wavelength,nm

Product IDPrice

1-3 pcs.λ/2 retardation, clear aperture

>18 mm

λ/4 retardation, clear aperture

>18 mm

266 2-CPW-ZO-L/2-0266 2-CPW-ZO-L/4-0266 210€343 2-CPW-ZO-L/2-0343 2-CPW-ZO-L/4-0343 210€355 2-CPW-ZO-L/2-0355 2-CPW-ZO-L/4-0355 210€400 2-CPW-ZO-L/2-0400 2-CPW-ZO-L/4-0400 210€473 2-CPW-ZO-L/2-0473 2-CPW-ZO-L/4-0473 210€515 2-CPW-ZO-L/2-0515 2-CPW-ZO-L/4-0515 210€532 2-CPW-ZO-L/2-0532 2-CPW-ZO-L/4-0532 210€589 2-CPW-ZO-L/2-0589 2-CPW-ZO-L/4-0589 210€633 2-CPW-ZO-L/2-0633 2-CPW-ZO-L/4-0633 210€780 2-CPW-ZO-L/2-0780 2-CPW-ZO-L/4-0780 210€800 2-CPW-ZO-L/2-0800 2-CPW-ZO-L/4-0800 210€852 2-CPW-ZO-L/2-0852 2-CPW-ZO-L/4-0852 210€940 2-CPW-ZO-L/2-0940 2-CPW-ZO-L/4-0940 210€980 2-CPW-ZO-L/2-0980 2-CPW-ZO-L/4-0980 210€

1030 2-CPW-ZO-L/2-1030 2-CPW-ZO-L/4-1030 210€1064 2-CPW-ZO-L/2-1064 2-CPW-ZO-L/4-1064 210€1122 2-CPW-ZO-L/2-1122 2-CPW-ZO-L/4-1122 210€1319 2-CPW-ZO-L/2-1319 2-CPW-ZO-L/4-1319 210€1550 2-CPW-ZO-L/2-1550 2-CPW-ZO-L/4-1550 210€

Catalog Items

Features

• Waveplates are made from excellent quality laser grade crys-talline quartz material

• We specialize in air-spaced zero-order waveplates• Dual wavelength waveplates are also available

Miscellaneous

• Custom design waveplates are available in small and mass pro-duction quantities

• Mass production capabilities: 5’000 pieces per month • Many waveplates are available from stock with fast delivery!• Dual wavelength waveplates are also available• Optically contacted waveplates for custom orders

* Contact ALTECHNA for larger quantity pricing [email protected]

LO crystalline quartz waveplates (mounted in 25.4 mm metal mount)

Wavelength,nm

Product IDPrice

1-3 pcs.λ/2 retardation, clear aperture

>18 mm


>18 mm

266 2-CPW-LO-L/2-0266 2-CPW-LO-L/4-0266 125€343 2-CPW-LO-L/2-0343 2-CPW-LO-L/4-0343 125€355 2-CPW-LO-L/2-0355 2-CPW-LO-L/4-0355 125€400 2-CPW-LO-L/2-0400 2-CPW-LO-L/4-0400 125€473 2-CPW-LO-L/2-0473 2-CPW-LO-L/4-0473 125€515 2-CPW-LO-L/2-0515 2-CPW-LO-L/4-0515 125€532 2-CPW-LO-L/2-0532 2-CPW-LO-L/4-0532 125€589 2-CPW-LO-L/2-0589 2-CPW-LO-L/4-0589 125€633 2-CPW-LO-L/2-0633 2-CPW-LO-L/4-0633 125€780 2-CPW-LO-L/2-0780 2-CPW-LO-L/4-0780 125€800 2-CPW-LO-L/2-0800 2-CPW-LO-L/4-0800 125€852 2-CPW-LO-L/2-0852 2-CPW-LO-L/4-0852 125€940 2-CPW-LO-L/2-0940 2-CPW-LO-L/4-0940 125€980 2-CPW-LO-L/2-0980 2-CPW-LO-L/4-0980 125€

1030 2-CPW-LO-L/2-1030 2-CPW-LO-L/4-1030 125€1064 2-CPW-LO-L/2-1064 2-CPW-LO-L/4-1064 125€1122 2-CPW-LO-L/2-1122 2-CPW-LO-L/4-1122 125€1319 2-CPW-LO-L/2-1319 2-CPW-LO-L/4-1319 125€1550 2-CPW-LO-L/2-1550 2-CPW-LO-L/4-1550 125€


Material Crystalline quartz

AR coatings R < 0.2% at each surface

Retardation tolerance λ/500 @ 20 °C

Wavefront distortion λ/10

Surface quality 20-10 Scratch & Dig

Parallelism error < 3 arcsec

Laser damage threshold 5 J/cm2 for 10 ns pulses @ 1064 nm typical

MountingMounted in 25.4 mm black anodized metal mount


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HIGH POWER WAVEPLATES

Description

Epoxy free waveplates for high power applications withstand energy density up to >20 J/cm2 @ 1064nm for 10ns pulses with 10 Hz pulse repetition rate. Unique design minimizes adjust-ment sensitivity because of wide acceptance angle. Since usage temperature bandwidth is more than 200 K, waveplate can be used in hazardous conditions with no additional losses. Wave-plate order depends on design wavelength and retardation.

Features

• High damage threshold• High extinction ratio• Wide acceptance angle• Wide temperature bandwidth • Wide spectral bandwidth• Extremely useful in UV applications

Related products


Material Crystalline quartz or MgF2

AR coatings R<0.2%

Surface finish 20-10 Scratch & Dig

Retardation tolerance λ/500

Wavefron distortion λ/10

Acceptance angle 11.37 deg

Damage threshold >20 J/cm2 @ 1064nm 10ns 10Hz

• 5PH50 - polarizer holders (page 220)

• 5APH59T-1 - adjustable polarizer mounts (page 218)

• Polarizing cubes for high power applications (page 113)

• Brewster type thin film polarizers (page 109)

• Broadband (ultrafast) thin film polarizers (page 111)


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Catalog Items

Clear aperture, mm

Retardation Wavelength, nm Waveplate order Product ID Price

>18 λ/2 266 1st 2-CPW-TFO-L/2-0266 350€>18 λ/2 343 1st 2-CPW-TFO-L/2-0343 350€>18 λ/2 355 1st 2-CPW-TFO-L/2-0355 350€>18 λ/2 400 1st 2-CPW-TFO-L/2-0400 350€>18 λ/2 515 1st 2-CPW-TFO-L/2-0515 350€>18 λ/2 532 1st 2-CPW-TFO-L/2-0532 350€>18 λ/2 589 0 2-CPW-TZO-L/2-0589 350€>18 λ/2 780 0 2-CPW-TZO-L/2-0780 350€>18 λ/2 800 0 2-CPW-TZO-L/2-0800 350€>18 λ/2 940 0 2-CPW-TZO-L/2-0940 350€>18 λ/2 980 0 2-CPW-TZO-L/2-0980 350€>18 λ/2 1030 0 2-CPW-TZO-L/2-1030 350€>18 λ/2 1064 0 2-CPW-TZO-L/2-1064 350€>18 λ/2 1550 0 2-CPW-TZO-L/2-1550 350€>18 λ/4 266 3rd 2-CPW-TTO-L/4-0266 350€>18 λ/4 343 2nd 2-CPW-TSO-L/4-0343 350€>18 λ/4 355 2nd 2-CPW-TSO-L/4-0355 350€>18 λ/4 400 2nd 2-CPW-TSO-L/4-0400 350€>18 λ/4 515 2nd 2-CPW-TSO-L/4-0515 350€>18 λ/4 589 1st 2-CPW-TFO-L/4-0589 350€>18 λ/4 780 1st 2-CPW-TFO-L/4-0780 350€>18 λ/4 800 1st 2-CPW-TFO-L/4-0800 350€>18 λ/4 940 1st 2-CPW-TFO-L/4-0940 350€>18 λ/4 980 1st 2-CPW-TFO-L/4-0980 350€>18 λ/4 1030 1st 2-CPW-TFO-L/4-1030 350€>18 λ/4 1064 0 2-CPW-TZO-L/4-1064 350€>18 λ/4 1550 0 2-CPW-TZO-L/4-1550 350€>18 λ/4 532 1st 2-CPW-TFO-L/4-0532 350€


If you do not find suitable waveplate for your application please contact us and we guaranty to provide a solution for you


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Material Quartz + MgF2

Dimension tolerance +0.00/-0.2 mm

Retardation tolerance λ/100

Clear aperture >90% central area

Wavefront distortion λ/4 @ 632.8 nm


Parallelism error <30 arcsec


AR coatings BBAR coated by default

Mounting Mounted in 25.4 mm black anodized metal mount

ACHROMATIC (BROADBAND) WAVEPLATESDescription

An achromatic waveplate (AWP) is a pair of crystal quartz and magnesium fluoride plates.

Because of the difference in dispersion in these uniaxial positive crystals it is possible to calculate thickness of each plate so that birefringent phase shift in assembly changes very slowly over a certain wavelength range. This is a way to obtain achromatic zero order waveplates. Such AWPs are necessary for various devices and may replace a number of ordinary quartz waveplates operating at a single wavelength only. We can offer series of Achromatic Waveplates with phase shifts shown in graphs below.

TYPICAL RETARDATION CURVES FOR 650-1100NMACHROMATIC WAVEPLATES

Retardation for 2-APW-L/2-012C

Retardation for 2-APW-L/4-012C


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Catalog Items

Wavelength,nm

Product IDPriceλ/2 retardation,

clear aperture >8 mm λ/4 retardation,

clear aperture >8 mm450-650 2-APW-L/2-008A 2-APW-L/4-008A 370€550-750 2-APW-L/2-008B 2-APW-L/4-008B 370€

650-1100 2-APW-L/2-008C 2-APW-L/4-008C 370€900-2100 2-APW-L/2-008D 2-APW-L/4-008D 370€

λ/2 retardation, clear aperture >12 mm


450-650 2-APW-L/2-012A 2-APW-L/4-012A 415€550-750 2-APW-L/2-012B 2-APW-L/4-012B 415€




450-650 2-APW-L/2-018A 2-APW-L/4-018A 640€550-750 2-APW-L/2-018B 2-APW-L/4-018B 640€


Features

• Operates over broad wavelength range• We specialize in air-spaced achromatic aaveplates• All waveplates are BBAR coated and mounted by default

Miscellaneous


• Mass production capabilities: 2’000 pieces per month


If you do not find suitable waveplate for your application please contact us and we guaranty to provide a solution for you

Related products and accessories


• 5PH51 - polarizer holder (page 219)


• High power laser glan polarizers (page 111)


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MID-IR WAVEPLATES

Description

Zero order half waveplates and quarter waveplates from cad-mium thiogallate (CdGa2S4) with clear aperture from 10mm up to 18mm for the range 2,8 - 9,0 microns are now available from ALTECHNA.

Dielectric AR Coatings for the mid-IR range are also available in order to enhance the performance of the waveplates. The char-acteristic plate thickness is 0.5 – 0.9 mm. Generally, the wave-plates are mounted into a metal holder for easier handling and adjustment.


Material Cadmium thiogallate (CdGa2S4)

Characteristic thickness 0.5 - 0.9 mm

Clear aperture 10 mm

Surface flatness <λ/4 @ 632.8 nm

Wedge angle between faces1.5 - 3.0 arcmin; <20 arcsec available upon request

Transparency range 0.47 - 9.5 um

Birefringence (no-n

e) ~0.005 at IR

Refractive index no ~2.3

Thermal conductivity ~3 W/(m×K)

Damage threshold ~0.6 - 0.8 J/cm2 at 20 ns pulses

Diameter of the metal holder 25.4 mm

Features

• ZO waveplates for mid-IR applications (2.800-9.000 microns)• Custom size available

Miscellaneous


Catalog Items

Wave-length,

nm

Product IDPrice

*1-2 pcsfor

uncoated

Price*1-2 pcs

for AR/AR coated


>10 mm


>10 mm

2940 2-IRPW-ZO-L/2-2940 2-IRPW-ZO-L/4-2940 800€ 1080€

3000 2-IRPW-ZO-L/2-3000 2-IRPW-ZO-L/4-3000 800€ 1080€

3500 2-IRPW-ZO-L/2-3500 2-IRPW-ZO-L/4-3500 800€ 1080€

4000 2-IRPW-ZO-L/2-4000 2-IRPW-ZO-L/4-4000 800€ 1080€

4500 2-IRPW-ZO-L/2-4500 2-IRPW-ZO-L/4-4500 800€ 1080€

5000 2-IRPW-ZO-L/2-5000 2-IRPW-ZO-L/4-5000 800€ 1080€

5500 2-IRPW-ZO-L/2-5500 2-IRPW-ZO-L/4-5500 800€ 1080€

6000 2-IRPW-ZO-L/2-6000 2-IRPW-ZO-L/4-6000 800€ 1080€

6500 2-IRPW-ZO-L/2-6500 2-IRPW-ZO-L/4-6500 800€ 1080€

7000 2-IRPW-ZO-L/2-7000 2-IRPW-ZO-L/4-7000 800€ 1080€

7500 2-IRPW-ZO-L/2-7500 2-IRPW-ZO-L/4-7500 800€ 1080€

8000 2-IRPW-ZO-L/2-8000 2-IRPW-ZO-L/4-8000 800€ 1080€

9000 2-IRPW-ZO-L/2-9000 2-IRPW-ZO-L/4-9000 800€ 1080€


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S-waveplate is a super-structured waveplate which converts lin-ear polarization to radial or azimuthal polarization. Product is unique for its high damage threshold 10 times exceeding alter-native devices: according to ISO 11254 – 2 is θ 1000-on-1 = 22.80 ± 2.74 J/cm2, at λ = 1064 nm, τ = 3.5 ns,

f = 10 Hz. High results achieved because converter is fabricated inside a bulk of UVFS glass.

Radial (left) and azimuth (right) polarization beam intensity dis-tributions (black arrows show electromagnetic field orientation).

Features

• Convertslinearpolarizationtoradialorazimuthal• Canbeusedtocreateanopticalvortex• Highdamagethreshold• Nearly100%efficiency inpolarizationconversion fordedicat-

ed wavelengths• 50-90%transmission(ARcoatingsapplicable)• Largeaperturepossible(upto10mmorbigger;standardis6

mm)• Nogluedcomponents–moreresistanttoheat• No“ineffectivecenter”proble• Nosegmentstitching

SPECIAL OPTICSS-WAVEPLATE

Benefits for laser micromachining

Radial polarization enables focusing of laser beam into smaller spot size (with high NA>0.9 optics).

For polarization direction sensitive applications radial/azimuth polarization allows same machining properties in all directions). It is also applicable in optical tweezers, STED microscopy or any other depletion application.

Catalog Items

Product IDOperation

Wavelength, nmTransmission

ClearAperture, mm

Price*1-9 pcs

RPC-488-2 488 ±15 >40 % 2 600€

RPC-488-6 488 ±15 >40 % 6 1200€

RPC-515-02 515 ±20 >45 % 2 600€

RPC-515-04 515 ±20 >45 % 4 900€

RPC-515-06 515 ±20 >45 % 6 1200€

RPC-632-2 632 ±20 > 50 % 2 700€

RPC-632-4 632 ±20 > 50 % 4 1200€

RPC-632-6 632 ±20 > 50 % 6 1900€

RPC-800-02 800 ±25 >55% 2 700€

RPC-800-04 800 ±25 >55% 4 1200€

RPC-800-06 800 ±25 >55% 6 1900€

RPC-800-10 800 ±25 >55% 10 5000€

RPC-1030-02 1030 ±35 >65% 2 700€

RPC-1030-04 1030 ±35 >65% 4 1000€

RPC-1030-06 1030 ±35 >65% 6 1900€

RPC-1030-10 1030 ±35 >65% 10 5000€

RPC-1550-02 1550 ±40 >75% 2 800€

RPC-1550-04 1550 ±40 >75% 4 1300€

RPC-1550-06 1550 ±40 >75% 6 2400€

* Custom wavelength and size converters are available on request.


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BREWSTER TYPE THIN FILM POLARIZERS

Description

Brewster type thin film polarizers are used for high energy ap-plications.

They have high damage threshold reaching 10 J/cm² @ 1064 nm for 8 ns. Brewster polarizers are used as an alternative to Glan-Taylor laser polarizing prisms or cube polarizing beamsplitters.

Typically, BK7 or UVFS dielectric coated brewster type thin film polarizers separate the s- and p-polarization components of high energy laser beams and are intended for intra and extra cavity usage.

Typical polarization ratio Tp/T

s is 200:1 and it is achieved at 56°

AOI (Brewster angle). For optimal transmission Brewster type thin film polarizer should be mounted in an appropriate holder for angular adjustment.


Material BK7, UVFS

Diameter tolerance +0.00/-0.12 mm

Thickness tolerance ±0.2 mm

Clear aperture >90%


Surface flatness λ/10 @ 632.8 nm


Extinction ratio Tp/T

s>200:1

Typical transmission Tp>95%

Typical reflection Rs>99,5%


Features

• Efficiently separates the s- and p- polarization components• Optimised for popular laser wavelengths • Many brewster thin film polarizers are available from stock

with fast delivery!

Miscellaneous

• Custom design brewster thin film polarizers are available in small and mass production quantities

• Mass production capabilities: 3’000 pieces per month • Brewster thin film polarizers with dimensions up to 200x150

mm are available


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• Beamsplitter / mirror mounts 5BM131 and 5BM141 (page 220)

• 4PH132 - universal plate holder (page 214)

• Crystalline quartz waveplates (page 100)

• 3AM-1 – polarizers holder (CA 12mm; accepts D25.4 and 20x40x5mm optics)

• Watt Pilot (page 177)• Motorized Watt Pilot (page 183)

Related products and accessoriesCatalog ItemsWavelength, nm

Substrate material

Dimensions, mm Product ID Price

266 UVFSØ25.4x3 2-BFP-0266-0254 119€Ø50.8x6 2-BFP-0266-0508 180€20x40x5 2-BFP-0266-2040 185€





532 BK7Ø25.4x3 2-BFP-0532-0254 85€Ø50.8x8 2-BFP-0532-0508 120€20x40x5 2-BFP-0532-2040 110€


780-820 (centered @ 800nm)

UVFSØ25.4x3 2-BFP-0800-A-0254 119€Ø50.8x6 2-BFP-0800-A-0508 150€20x40x5 2-BFP-0800-A-2040 150€

795-805 (centered @ 800nm)

UVFSØ25.4x3 2-BFP-0800-0254 94€Ø50.8x6 2-BFP-0800-0508 150€20x40x5 2-BFP-0800-2040 130€



1020-1040 (centered @

1030nm)UVFS

Ø25.4x3 2-BFP-1030-0254 119€Ø50.8x6 2-BFP-1030-0508 150€20x40x5 2-BFP-1030-2040 150€




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BROADBAND (ultrafast) THIN FILM POLARIZERS

Description

Broadband (ultrafast) thin film polarizers are used for femtosec-ond lasers.

PLEASE NOTE: The optimal working angle is AOI=72° (±2°).

We are offering 4 types of broadband (Ultrafast) thin film polariz-ers. Polarizers work by transmitting p polarization and reflecting s polarization.

TRANSMISSION POLARIZERS - have polarizing coatings on both sides of the polarizer. They can be optimized for highest trans-mission of p polarization T

p > 94% or best contrast of polariza-

tions Tp:T

s>20:1.

REFLECTION POLARIZERS - have polarizing coating on the in-put face while the output face is AR coated for both s and p polarizations. They can be optimized for highest reflection of s polarization R

s > 98% or best contrast of polarizations R

s:R

p>60:1.

Moreover, the AR coated side of a polarizer can have wedge to minimize ghosting. Standard thin film polarizers are designed for optimum performance in the 750 - 850 nm or 980 - 1090 nm range. Design of custom wavelength range is also available.

Features

• Efficiently separates the s- and p- polarization components• Optimised for popular laser wavelengths • Many broadband (ultrafast) thin film polarizers are available

from stock with fast delivery!


Substrate material UVFS

Diameter tolerance +0.00/-0.12 mm

Thickness tolerance ±0.2 mm

Clear aperture >90%



Angle of incidence 72°




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Catalog Items

2-UFP-0800-xxxx-T1

2-UFP-0800-xxxx-T2

2-UFP-0800-xxxx-R2

2-UFP-0800-xxxx-R1

TRANSMISSION TYPE broadband (ultrafast) thin film polarizers

Wavelength, nmExtinction ratio T

p/T

s

Transmis-sion, %

Dimensions, mmW x L x Thickness

Product ID Price

750-850(centered @ 800nm)Contrast optimized

>20:1Tp>85%Ts<4%

Ø25.4x3 2-UFP-0800-0254-T2 235€20x60x2 2-UFP-0800-2060-T2 290€

50x160x3 2-UFP-0800-5016-T2 730€

750-850(centered @ 800nm)

Tp optimized

>9:1Tp>94%Ts<10%

Ø25.4x3 2-UFP-0800-0254-T1 210€20x60x2 2-UFP-0800-2060-T1 275€

50x160x3 2-UFP-0800-5016-T1 710€

980-1090(centered @ 1030nm)

Contrast optimized>20:1

Tp>85%Ts<4%

Ø25.4x3 2-UFP-1030-0254-T2 225€20x60x2 2-UFP-1030-2060-T2 290€

50x160x3 2-UFP-1030-5016-T2 730€

980-1090(centered @ 1030nm)

Tp

optimized>9:1

Tp>94%Ts<10%

Ø25.4x3 2-UFP-1030-0254-T1 210€20x60x2 2-UFP-1030-2060-T1 275€

50x160x3 2-UFP-1030-5016-T1 710€

REFLECTION TYPE broadband (ultrafast) thin film polarizers

Wavelength, nmExtinction ratio R

s/R

p

Reflec-tion,%

Dimensions, mmW x L x Thickness

Product ID Price

750-850(centered @ 800nm)

Rs optimized

>5:1Rs>98%Rp<20%

Ø25.4x3 2-UFP-0800-0254-R1 235€20x60x5 2-UFP-0800-2060-R1 290€

50x160x8 2-UFP-0800-5016-R1 730€

750-850(centered @ 800nm)Contrast optimized

>60:1Rs>85%Rp<1%

Ø25.4x3 2-UFP-0800-0254-R2 210€

20x60x5 2-UFP-0800-2060-R2 275€50x160x8 2-UFP-0800-5016-R2 710€

980-1090(centered @ 1030nm)

Rs optimized

>5:1 Rs>98%Rp<20%

Ø25.4x3 2-UFP-1030-0254-R1 225€20x60x5 2-UFP-1030-2060-R1 290€

50x160x8 2-UFP-1030-5016-R1 730€

980-1090(centered @ 1030nm)

Contrast optimized>60:1

Rs>85%Rp<1%

Ø25.4x3 2-UFP-1030-0254-R2 210€

20x60x5 2-UFP-1030-2060-R2 275€50x160x8 2-UFP-1030-5016-R2 710€


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POLARIZING CUBES

Description

Polarizing cubes for specified wavelength (250-2200 nm) AR coated on four input and output working surfaces. Polarizing beamsplitter cubes split randomly polarized beams into two orthogonal, linearly polarized components: s polarized light is reflected at a 90° angle while p-polarized light is transmitted.

Polarizing cubes for medium power applications

Each beamsplitter consists of a pair of high precision right an-gle prisms cemented together with a dielectric coating on the hypotenuse of one of the prisms. Typical damage threshold of these cubes is >0,3 J/cm2 @ 1064 nm 10 ns at 20 Hz.

Polarizing cubes for high power applications

OPTICALLY CONTACTED polarizing beamsplitter cubes used for HIGH POWER applications can withstand energy fluencies up to 20 J/cm2 @ 1064 nm for 10 ns pulses at 20 Hz.


Material BK7, UVFS, SF glasses

Dimension tolerances +0.00/-0.3 mm

Clear aperture >90% of the face size


Surface flatness λ/4 at 632.8 nm

Beam deviation <3 arcmin

Laser damage treshold, (10 ns pulses @ 1064 nm)

>0.3 J/cm2 for cemented cubes

~10 J/cm2 for optically contacted cubes

Features

• Optimized for popular laser wavelengths • Dual wavelength polarizing cubes are also available• All polarizing cubes are AR coated• Many Polarizing cubes are available from stock with fast

delivery!


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If you do not find suitable size substrate for your application please contact us and we guaranty to provide a solution for you

• 5OM37 - two angular fine adjustment mounts (page 223)

• Crystalline quartz waveplates (page 100)

• Watt Pilot (page 177)


Wave-length,

nm

Dimensions, mm

Reflections-pol. %

Transmissionp-pol. %

Product ID Price

35512.7 x 12.7 x 12.7 >99% >90% 2-PCB-A-0125 295€25.4 x 25.4 x 25.4 >99% >90% 2-PCB-A-0200 320€

40012.7 x 12.7 x 12.7 >99% >90% 2-PCB-B-0125 295€25.4 x 25.4 x 25.4 >99% >90% 2-PCB-B-0200 320€

450-65012.7 x 12.7 x 12.7 >99.5% >95% 2-PCB-C-0125 94€25.4 x 25.4 x 25.4 >99.5% >95% 2-PCB-C-0200 100€

53212.7 x 12.7 x 12.7 >99.8% >97% 2-PCB-D-0125 94€25.4 x 25.4 x 25.4 >99.8% >97% 2-PCB-D-0200 110€

63312.7 x 12.7 x 12.7 >99.8% >97% 2-PCB-E-0125 94€25.4 x 25.4 x 25.4 >99.8% >97% 2-PCB-E-0200 110€

700-90012.7 x 12.7 x 12.7 >99.5% >95% 2-PCB-F-0125 100€

15 x 15 x 15 >99.5% >95% 2-PCB-F-0150 110€25.4 x 25.4 x 25.4 >99.5% >95% 2-PCB-F-0200 115€

78012.7 x 12.7 x 12.7 >99.8% >97% 2-PCB-G-0125 94€25.4 x 25.4 x 25.4 >99.8% >97% 2-PCB-G-0200 110€

85012.7 x 12.7 x 12.7 >99.8% >97% 2-PCB-H-0125 94€25.4 x 25.4 x 25.4 >99.8% >97% 2-PCB-H-0200 110€

1020-110012.7 x 12.7 x 12.7 >99.5% >97% 2-PCB-J-0125 100€25.4 x 25.4 x 25.4 >99.5% >97% 2-PCB-J-0200 115€

106412.7 x 12.7 x 12.7 >99.8% >97% 2-PCB-K-0125 94€25.4 x 25.4 x 25.4 >99.8% >97% 2-PCB-K-0200 110€

131012.7 x 12.7 x 12.7 >99.8% >97% 2-PCB-L-0125 94€25.4 x 25.4 x 25.4 >99.8% >97% 2-PCB-L-0200 110€

155012.7 x 12.7 x 12.7 >99.8% >97% 2-PCB-M-0125 94€25.4 x 25.4 x 25.4 >99.8% >97% 2-PCB-M-0200 110€

Catalog Items

OPTICALLY CONTACTED polarizing cubes for high power applications

Wavelength, nm Dimensions, mmReflection

s-pol, %Transmission

p-pol, %Product ID Price

345-365 (centered @ 355 nm)

12.7 x 12.7 x 12.7 >99.5% >97% 2-HPCB-A-0125 310€

510-550(centered @ 532 nm)

12.7 x 12.7 x 12.7 >99.5% >97% 2-HPCB-B-0125 260€

1020-1090(centered @ 1064 nm)

12.7 x 12.7 x 12.7 >99.5% >97% 2-HPCB-C-0125 260€

1510-1580(centered @ 1550 nm)

12.7 x 12.7 x 12.7 >99.5% >97% 2-HPCB-D-0125 260€


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If you do not find suitable high power Glan laser polarizer for your application please contact us and we guaranty to provide a solution for you

HIGH POWER GLAN LASER POLARIZERSDescription

High Power Glan Laser polarizer produces linear polarized light from unpolarized input and is made of a higher grade calcite. The polarizer has two escape windows to allow the rejected beams to escape. Its entrance and exit faces are polished using deep grinding and polishing technique to minimize scattering from the surface.


Material a-BBO, Calcite or YVO4

Wavelength range

a-BBO: 220 - 350 nm, 350 - 700 nm, 700 - 3000 nm, Calcite: 350 - 2200 nm, YVO4: 500 - 4000 nm

Extinction ratioa-BBO: <5×10-6, Calcite: <5×10-5, YVO

4: <5×10-6

Surface quality 20-10 Scratch and Dig

Beam deviation < 3 arcmin


Damage threshold >500 MW/cm2

Coating Single layer MgF2

Mount Black anodized aluminum

Features

• Broadband high power polarizers for visible or near IR wave-lengths

• Air-spaced• Close to brewster ’s angle cutting• High polarization purity• Short length• Double escape windows for intracavity use

Miscellaneous

• Other size, better quality, different spectral ranges, housing or AR coatings are available on request


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Calcite Glan laser polarizer

Wavelength, nm Extinction ratioAngularfield, °

C.A.Øa (mm)

O.D.Ød (mm)

L±0.1 (mm) Product ID Price

350-2200 <5×10-5 >7.7

8.0 25.4 24.5 2-GL-3522-1 330€10.0 25.4 26.2 2-GL-3522-2 375€

12.70 25.4 27.5 2-GL-3522-3 450€15.0 30.0 33.0 2-GL-3522-4 520€20.0 38.0 42.3 2-GL-3522-5 810€

a-BBO Glan laser polarizer


C.A.Øa (mm)

O.D.Ød (mm)

L±0.1(mm)

Product ID Price

220-350 <5×10-6 >6.0

8.0 25.4 30.4 2-GL-2235-1 470€10.0 25.4 31.0 2-GL-2235-2 530€

12.70 25.4 31.5 2-GL-2235-3 615€15.0 30.0 38.6 2-GL-2235-4 720€20.0 38.0 48.9 2-GL-2235-5 1000€

350-700 <5×10-6 >6.0

8.0 25.4 25.0 2-GL-3570-1 470€10.0 25.4 26.0 2-GL-3570-2 530€

12.70 25.4 27.0 2-GL-3570-3 615€15.0 30.0 33.4 2-GL-3570-4 720€20.0 38.0 41.7 2-GL-3570-5 1000€

700-3000 <5×10-6 >6.0

8.0 25.4 24.7 2-GL-7030-1 470€10.0 25.4 25.9 2-GL-7030-2 530€

12.70 25.4 27.0 2-GL-7030-3 615€15.0 30.0 33.0 2-GL-7030-4 720€20.0 38.0 43.6 2-GL-7030-5 1000€

YVO4 Glan laser polarizer


C.A.Øa (mm)

O.D.Ød (mm)

L±0.1(mm)

Product ID Price

500-4000 <5×10-6 >6.58.0 25.4 20 2-GL-5040-1 450€

10.0 25.4 23 2-GL-5040-2 525€15.0 30.0 29 2-GL-5040-3 780€

Catalog Items

• 5PH51 - polarizer holder (page 219) • 5APH59T-1 - adjustable polarizer mounts (page 218)


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GLAN TAYLOR POLARIZERS

Description

The device produces linearly polarized light from an unpolar-ized input.

A Glan Taylor prism consists of two prisms separated by an air gap. The transmitted beam of extraordinary polarization is used. The rejected beam is absorbed by black glass plates cemented to the prisms.


Material a-BBO, Calcite or YVO4

Wavelength range

a-BBO: 220 - 350 nm, 350 - 700 nm, 700 - 3000 nm, Calcite: 350 - 2200 nm, YVO4: 500 - 4000 nm

Extinction ratioa-BBO: <5×10-6, Calcite: <5×10-5, YVO

4: <5×10-6







Miscellaneous

• Other size, better quality, different spectral ranges or AR coat-ings are available on request

Features

• Air-spaced, medium power polarizers for visible or near IR wavelengths

• Rejected beam absorbed internally, <5x10-6 extinction ratio• Close to brewster ’s angle cutting• High polarization purity• Short length


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If you do not find suitable Glan Taylor polarizer for your application please contact us and we guaranty to provide a solution for you


Calcite Glan Taylor polarizerWavelength,

nmExtinction

ratioAngularfield, °

C.A.Øa (mm)

O.D.Ød (mm)

L±0.1(mm)

Product ID Price

350-2200 <5×10-5 >7.7

8.0 25.4 17.0 2-GT-3522-1 285€10.0 25.4 19.0 2-GT-3522-2 360€

12.70 25.4 21.0 2-GT-3522-3 410€15.0 30.0 23.0 2-GT-3522-4 475€20.0 38.0 29.0 2-GT-3522-5 795€

a-BBO Glan Taylor polarizerWavelength,

nmExtinction


C.A.Øa (mm)

O.D.Ød (mm)

L±0.1(mm)

Product ID Price

220-350 <5×10-6 >6.0

8.0 25.4 17.0 2-GT-2235-1 395€10.0 25.4 19.0 2-GT-2235-2 485€

12.70 25.4 21.0 2-GT-2235-3 590€15.0 30.0 23.0 2-GT-2235-4 700€20.0 38.0 29.0 2-GT-2235-5 980€

350-700 <5×10-6 >6.0

8.0 25.4 17.0 2-GT-3570-1 395€10.0 25.4 19.0 2-GT-3570-2 485€

12.70 25.4 21.0 2-GT-3570-3 590€15.0 30.0 23.0 2-GT-3570-4 700€20.0 38.0 29.0 2-GT-3570-5 980€

700-3000 <5×10-6 >6.0

8.0 25.4 17.0 2-GT-7030-1 395€10.0 25.4 19.0 2-GT-7030-2 485€

12.70 25.4 21.0 2-GT-7030-3 590€15.0 30.0 23.0 2-GT-7030-4 700€20.0 38.0 29.0 2-GT-7030-5 980€

YVO4 Glan Taylor polarizerWavelength,

nmExtinction


C.A.Øa (mm)

O.D.Ød (mm)

L±0.1(mm)

Product ID Price

500-4000 <5×10-6 >6.0

8.0 25.4 15 2-GT-5040-1 360€10.0 25.4 17 2-GT-5040-2 460€12.7 25.4 18.5 2-GT-5040-3 570€

15.0 30.0 20.0 2-GT-5040-4 675€

Catalog Items




• High power laser glan polarizers (page 115)


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GLAN THOMPSON POLARIZERS

Description

A Glan Thompson prism is a birefringent polarizing element which consists of two calcite prisms cemented together.

Because of the cement it has higher transmission than a Glan Taylor type polarizer due to the reduced reflection losses at the hypotenuse interface but limited useful UV spectral range. The transmitted beam of extraordinary polarization is used. Side fac-es are black painted to absorb the rejected beam.


Material Calcite

Wavelength range 350-2200 nm

Extinction ratio 5×10-5







Features

• Broadband low power polarizers for UV, visible or near IR wave-lengths

• Large acceptance angle• High polarization purity

Miscellaneous


Catalog Items


C.A.Øa (mm)

O.D.Ød (mm)

L±0.1(mm)

Product ID Price

350-2200 <5×10-5 >158.0 25.4 28.0 2-GTH-3522-1 370€

10.0 25.4 33.0 2-GTH-3522-2 425€12.70 25.4 40.0 2-GTH-3522-3 490€


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WOLLASTON POLARIZERS

Description

Wollaston prism is an optical device that separates unpolarized light into two orthogonal, linearly polarized outgoing beams.

The device consists of two birefringent prisms cemented to-gether. Wollaston polarizers deviate the two emerging beams by nearly equal amounts in opposite directions.


Material Calcite, YVO4 and quartz

Wavelength rangeCalcite: 350 - 2200 nm,YVO4: 500 - 4000 nm,Quartz: 200 - 2300 nm.

Extinction ratioCalcite: <5×10-5, YVO4: <5×10-6, Quartz: <5×10-4







Features

• Wide wavelength range• Low power application• Broadband 104 : 1 extinction ratio

Miscellaneous



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If you do not find suitable Wollaston polarizer for your application please contact us and we guaranty to provide a solution for you

Related ProductsQuartz Wollaston polarizerWavelength,

nmExtinction


C.A.Øa (mm)

O.D.Ød (mm)

L±0.1(mm)

Product ID Price

200-2300 <5×10-42.0 @

980nm

8.0 25.4 26.0 2-WP-2023-1 280€10.0 25.4 28.0 2-WP-2023-2 325€

12.70 25.4 33.0 2-WP-2023-3 375€15.0 30.0 38.0 2-WP-2023-4 430€20.0 38.0 48.0 2-WP-2023-5 670€

Calcite Wollaston polarizer

Wavelength, nm

Extinction ratio

Angu-lar

field, °

C.A.Øa (mm)

O.D.Ød (mm)

L±0.1(mm)

Product ID Price

350-3000 <5×10-4 16.0 @ 980nm

8.0 25.4 17.0 2-WP-3530-1 315€10.0 25.4 19.0 2-WP-3530-2 360€

12.70 25.4 21.0 2-WP-3530-3 450€15.0 30.0 23.0 2-WP-3530-4 510€20.0 38.0 29.0 2-WP-3530-5 880€

YVO4 Wollaston polarizerWavelength,

nmExtinction


C.A.Øa (mm)

O.D.Ød (mm)

L±0.1(mm)

Product ID Price

500-4000 <5×10-5 20.0 @ 1550nm

8.0 25.4 17.0 2-WP-5040-1 385€10.0 25.4 19.0 2-WP-5040-2 480€

12.70 25.4 21.0 2-WP-5040-3 560€15.0 30.0 23.0 2-WP-5040-4 600€20.0 38.0 29.0 2-WP-5040-5 970€

Catalog Items



• 5APH59T-1 - adjustable polarizer (page 218)


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BEAM DISPLACERS

Description

The device produces two parallel orthogonally polarized beams from an unpolarized input.

The displacement between the ordinary and extraordinary po-larized beams can be found from an approximate formula d = 0.1 x L

Beamdisplacers with size A greater than 20 mm are available on special request.

Beamdisplacers can be made from crystal quartz and rutile as well.


Material Calcite, YVO4

Size A from 5 x 5 to 20 x 20 mm

Length L from 5 to 35 mm

Tolerance Size A: +0.00/-0.1 mm, length L: ±0.1 mm

Ordinary beam deviation <3 arcmin

Surface quality 60–40 Scratch & Dig


Coatings None. AR coatings available upon request

Features

• Splits a beam into two orthogonaly polarized parallel beams• Made from the finest optical grade natural calcite or YVO

4

Miscellaneous


Catalog Items

MaterialDimensions (A×A, mm)

Beam displace-ment (mm)

Product ID Price

Calcite

5×51 2-BD-CALC-55-1 175€2 2-BD-CALC-55-2 230€3 2-BD-CALC-55-3 290€

8×81 2-BD-CALC-88-1 215€2 2-BD-CALC-88-2 250€3 2-BD-CALC-88-3 280€

YVO4

5×51 2-BD-YVO4-55-1 190€2 2-BD-YVO4-55-2 240€3 2-BD-YVO4-55-3 300€

8×81 2-BD-YVO4-88-1 230€2 2-BD-YVO4-88-2 265€3 2-BD-YVO4-88-3 300€


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ROCHON POLARIZERS

Description

The device produces linearly polarized light from an unpolarized input. Alternative to the other types of Glan type polarizers.


Material YVO4 and Quartz

Wavelength rangeYVO

4: 500 - 4000 nm,

Quartz: 200 - 2300 nm.

Extinction ratioYVO

4: <5×10-6,

Quartz: <5×10-4.

Surface quality 20-10 Scratch and Dig

Beam deviation <3 arcmin



Coating Single Layer MgF2

Mount Black anodized aluminium

Features

• Wide wavelength range• High extinction ratio• High UV transmission• Large field angle

Miscellaneous

• Other size, better quality, different spectral ranges or AR coat-ings are available on request


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If you do not find suitable Rochon polarizer for your application please contact us and we guaranty to provide a solution for you


Quartz Rochon polarizerWavelength,

nmExtinction


C.A.Øa (mm)

O.D.Ød (mm)

L±0.1(mm)

Product ID Price

200-2300 <5×10-4 1.0 @ 980nm

8.0 25.4 26.0 2-RP-2023-1 375€10.0 25.4 28.0 2-RP-2023-2 450€

12.70 25.4 33.0 2-RP-2023-3 490€15.0 30.0 38.0 2-RP-2023-4 550€20.0 38.0 48.0 2-RP-2023-5 760€

YVO4 Rochon polarizer

Wavelength, nm

Extinction ratio

Angularfield, °

C.A.Øa (mm)

O.D.Ød (mm)

L±0.1(mm)

Product ID Price

500-4000 <5×10-5 6.0 @ 1550nm

8.0 25.4 17.0 2-RP-5040-1 475€10.0 25.4 19.0 2-RP-5040-2 580€

12.70 25.4 21.0 2-RP-5040-3 660€15.0 30.0 23.0 2-RP-5040-4 710€20.0 38.0 29.0 2-RP-5040-5 1080€

Catalog Items

• 5OM37 - two angular fine adjustment mounts (page 223)


LASER AND PASSIVE Q-SWITCH CRYSTALS

LASER CRYSTALS 126

•Ti:SAPPHIRE crystals 126

•Nd:YVO4 crystals 128

•Nd:YAG crystals 130

•Nd:YLF crystals 132

•Nd:KGW crystals 133

•Yb:KGW and Yb:KYW crystals 135

•Yb:YAG crystals 137

•Yb:CaF2 crystals 139

PASSIVE Q-SWITCH CRYSTALS 140

•Cr4+:YAG crystals 140

•V3+:YAG crystals 142

•Co:Spinel crystals 144

Please contact [email protected] if you are also interested in the following crystals:

Nd:glass, Nd:YAPEr:YAG, Er:KYW, Er:YVO4Er/Yb:GlassYb:YVO4, Ho:YLFCr:LiSAF

Visit www.altechna.com to see the latest news and regular updates.


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Orientation Optical axis C normal to rod axis

Ti2O3 concentration 0.03-0.25 wt %

Figure of merit (FOM) 60-300 depending on the Ti3+ concentration

Maximal sizes up to 50 mm dia and up to 50 mm length

End configurations Flat/Flat or Brewster/Brewster

Flatness λ/10 @ 632.8 nm

Parallelism error 10 arcsec

Surface finishing 10-5 Scratch & Dig

Wavefront Ddistortion λ/4 per Inch

Absorption @ 532 nm on crystal length

>90%

AR coatings None. AR coatings available upon request

Ti:SAPPHIRE LASER CRYSTALS

Titanium doped sapphire (Al2O

3:Ti3+) is widely used for generating

ultra short femtosecond pulses and wavelength tunable lasers. It has remarkably high gain. Ti:Sapphire crystals can be effectively pumped by short pulse flash lamps in powerful laser systems.

Also these crystals combine supreme physical and optical properties with the broadest lasing range. Its indefinitely long stability and useful lifetime are an additional advantage. Medical laser systems, LIDARs, laser spectroscopy, direct femtosecond pulse generation by Kerr-type mode-locking - these are a few of the existing and potential applications.


Description

Features

Miscellaneous

• Broad lasing range: 660-1050 nm band• Perfect for ultrashort pulse generation• High gain and high power lasing• High optical quality and bulk damage threshold

• Custom design production is also available• Different doping levels available• Mass production at 500 pieces per month available• Various end cuts available (plano/plano, wedge/wedge, brewster cut, etc.)• Various dielectric coatings are available. Complex coatings are realized with IBS technique


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If you do not find suitable crystal for your application please contact us and we guaranty to provide a solution for you


Aperture dimensions, mm Length, mm End surfaces Product ID Price

Ø6

5 Brewster Cut 3-TS-1-0605 970€10 Brewster Cut 3-TS-1-0610 1020€15 Brewster Cut 3-TS-1-0615 1100€20 Brewster Cut 3-TS-1-0620 1200€5 Right-angle Cut 3-TS-0-0605 970€

10 Right-angle Cut 3-TS-0-0610 1020€15 Right-angle Cut 3-TS-0-0615 1100€20 Right-angle Cut 3-TS-0-0620 1200€

6x6

5 Brewster Cut 3-TS-1-6605 970€10 Brewster Cut 3-TS-1-6610 1020€15 Brewster Cut 3-TS-1-6615 1100€20 Brewster Cut 3-TS-1-6620 1200€5 Right-angle Cut 3-TS-0-6605 970€

10 Right-angle Cut 3-TS-0-6610 1020€15 Right-angle Cut 3-TS-0-6615 1100€20 Right-angle Cut 3-TS-0-6620 1200€

Catalog Items

• Enhanced Watt Pilot (page 179)


• Autocorrelator (page 192)

• Wavelength separators (page 60)

• Laser beam visualizer (page 199)

• Laser crystal repolishing (page 261)


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Nd:YVO4 LASER

CRYSTALS

Nd:YVO4 is one of the best host crystals for diode pumped solid

state lasers.

Neodymium doped yttrium vanadate (Nd:YVO4) is widely used

as diode pumped solid state laser material. It has a high laser induced damage threshold, good mechanical and optical properties. Its large stimulated emission cross-section and high absorption of pump radiation make it a suitable crystal for pocket laser pointer.

Nd:YVO4 can produce IR, green or blue radiation with minor

difference in set-up’s. A broad absorption band centered at 807 nm and favorable mechanical properties make Nd:YVO

4 well

suited for compact, efficient, high power diode-pumped lasers. Natural birefringence gives rise to a highly polarized output at 1064.3 and 1342 nm.


Description

Features

Miscellaneous

• Wide absorption bandwidth• Low lasing threshold• High slope efficiency• Large luminescence cross-section• Linearly polarized emission and single-mode output


Standard optical axis orientation A-cut

Shape Rectangular only

Doping concentration 0.5-3.0 atm. %

Thickness range 0.5-30 mm

Length tolerance +0.00/-0.1 mm

Non-parallelism of end faces 10”

Surface finishing 10-5 Scratch & Dig


Chamfer <0.1 mm @ 45°


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Material Dimensions, mm Coatings Product IDPrice

*1-5pcs

Nd(0,5%):YVO4

3×3×4 HR@1064&532+HT@808/AR@1064&532 3-ND05YVO-01 330€3×3×6 HR@1064&532+HT@808/AR@1064&532 3-ND05YVO-02 340€

3×3×10 HR@1064&532+HT@808/AR@1064&532 3-ND05YVO-03 350€3×3×4 AR/AR@1064&808 3-ND05YVO-04 310€3×3×6 AR/AR@1064&808 3-ND05YVO-05 320€

3×3×10 AR/AR@1064&808 3-ND05YVO-06 330€

Nd(1%):YVO4

3×3×1 HR@1064&532+HT@808/AR@1064&532 3-ND10YVO-01 290€3×3×2 HR@1064&532+HT@808/AR@1064&532 3-ND10YVO-02 300€3×3×3 HR@1064&532+HT@808/AR@1064&532 3-ND10YVO-03 310€3×3×4 HR@1064&532+HT@808/AR@1064&532 3-ND10YVO-04 330€3×3×1 AR/AR@1064&808 3-ND10YVO-05 270€3×3×2 AR/AR@1064&808 3-ND10YVO-06 280€3×3×3 AR/AR@1064&808 3-ND10YVO-07 290€3×3×4 AR/AR@1064&808 3-ND10YVO-08 300€

Nd(2%):YVO4

3×3×1 HR@1064&532+HT@808/AR@1064&532 3-ND20YVO-01 290€3×3×2 HR@1064&532+HT@808/AR@1064&532 3-ND20YVO-02 300€3×3×3 HR@1064&532+HT@808/AR@1064&532 3-ND20YVO-03 310€3×3×1 AR/AR@1064&808 3-ND20YVO-04 270€3×3×2 AR/AR@1064&808 3-ND20YVO-05 280€3×3×3 AR/AR@1064&808 3-ND20YVO-06 290€

Nd(3%):YVO4

3×3×0,5 HR@1064&532+HT@808/AR@1064&532 3-ND30YVO-01 290€3×3×1 HR@1064&532+HT@808/AR@1064&532 3-ND30YVO-02 300€3×3×2 HR@1064&532+HT@808/AR@1064&532 3-ND30YVO-03 310€

3×3×0,5 AR/AR@1064&808 3-ND30YVO-04 270€3×3×1 AR/AR@1064&808 3-ND30YVO-05 280€3×3×2 AR/AR@1064&808 3-ND30YVO-06 290€

Catalog Items

• Laser beam visualizer (page 199)• Wavelength separator (page 60)

• Laser diodes (page 203)

• Optical coatings (pages 86-98)



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Doping concentration 0.5-1.1 atm. %

Orientation [111]

Wavefront distortion ≤λ/10 @ 632.8 nm

Extinction ratio ≥28 dB

Dimensional tolerancesDiameter: +0.00/-0.05 mm, Length: +0.00/-0.10 mm.

Parallelism error ≤15 arcsec

Perpendicularity ≤5 arcmin

Flatness ≤λ/10 @ 632.8 nm



AR coating reflectivity ≤0.2% @ 1064 nm

Nd:YAG LASER CRYSTALS

The Nd:YAG crystal is the most widely used solid-state laser material today. Good fluorescence lifetime, thermal conductivity and robust nature make Nd:YAG crystals suitable for high power continuous wave, high intensity Q-switched and single mode operation.

Now, we are able to supply consistently Nd:YAG rods with high optical homogeneity, high damage threshold, consistent performance and high processing accuracy.


Description

Features

Miscellaneous

• Wide absorption bandwidth• Low lasing threshold• High slope efficiency• Large luminescence cross-section• Linearly polarized emission and single-mode output

• Custom design production is also available• Different doping levels available• Rods with barrel grooving are available for better performance• Mass production at 2000 pcs/month available• Various end cuts available (plano/plano, wedge/wedge, brewster cut, etc.)• Various dielectric coatings are available. Complex coatings are realized with IBS technique• One of the best selling products in 2012!


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Material Dimensions, mm Coatings Product IDPrice

*1-3pcs

Nd(0,6%):YAG

Ø3×60 AR/AR@1064 3-ND06YAG-01 385€Ø4×80 AR/AR@1064 3-ND06YAG-02 430€Ø5×90 AR/AR@1064 3-ND06YAG-03 460€

Ø6×110 AR/AR@1064 3-ND06YAG-04 580€Ø7×125 AR/AR@1064 3-ND06YAG-05 900€Ø8×130 AR/AR@1064 3-ND06YAG-06 940€Ø9×150 AR/AR@1064 3-ND06YAG-07 2200€

Ø10×160 AR/AR@1064 3-ND06YAG-08 2350€

Nd(1,1%):YAG

3×3×2 HR@1064+HT@808/AR@1064 3-ND11YAG-10 230€3×3×3 HR@1064+HT@808/AR@1064 3-ND11YAG-11 230€3×3×4 HR@1064+HT@808/AR@1064 3-ND11YAG-12 230€3×3×5 HR@1064+HT@808/AR@1064 3-ND11YAG-13 230€3×3×2 AR/AR@1064&808 3-ND11YAG-14 210€3×3×3 AR/AR@1064&808 3-ND11YAG-15 210€3×3×4 AR/AR@1064&808 3-ND11YAG-16 210€3×3×5 AR/AR@1064&808 3-ND11YAG-17 210€Ø3×60 AR/AR@1064 3-ND11YAG-01 385€Ø4×80 AR/AR@1064 3-ND11YAG-02 430€Ø5×90 AR/AR@1064 3-ND11YAG-03 460€

Ø6×110 AR/AR@1064 3-ND11YAG-04 580€Ø7×125 AR/AR@1064 3-ND11YAG-05 900€Ø8×130 AR/AR@1064 3-ND11YAG-06 940€Ø9×150 AR/AR@1064 3-ND11YAG-07 2200€

Ø10×160 AR/AR@1064 3-ND11YAG-08 2350€

Catalog Items

• Safety goggles (page 200)



• Optical coatings (page 86-98)





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Nd:YLF CRYSTALS

Description

Nd:LiYF is laser material alternative to Nd:YAG. Nd:YLF emission wavelengths are 1053, 1047, 1313, 1324, and 1370nm. Main Nd:YLF advantage over Nd:YAG is higher pulse energy at low (<2kHz) repetition rate. Other differences are also worth of mentioning: weak thermal lensing, relatively broad fluorescence linewidth and naturally polarized oscillation. ALTECHNA provides Nd:YLF crystals which are selected to have low inhomogeneity over all aperture. Crystals with diameter 10 mm, length 120 mm and inhomogeneity ~1 - 3 ppm are available.

Features

• Low inhomogeneity• Apertures up to 20mm• Length up to 120mm• Barrel side can be optimized for better heat handeling


Catalog Items

Material Nd:LiYF4

Dopant concentration 0.4%~2% atm%

Surface finish 10-5 Scratch & Dig

Flatness λ/10 @ 632.8nm

Wavefront distortion up to λ/8 @ 632.8nm


Dimensional tolerances Diameter: +0.00/-0.05mm



Chamfer <0.1 mm @ 45

Barrel side fine grinded or chemically etched (for better heat handling)

Damage threshold 4-6J/cm2 with 3ns pulse in 2mm diameter

Material Dimenssions, mm

Coating Product ID Price 1-3 pcs

Nd(1.1%):YLF 6x6x70AR/AR@(790-810) + (1047-1053) nm

3-ND11YLF-6670 3100€

Nd(1.1%):YLF 4x4x12AR/AR@(790-810) + (1047-1053) nm

3-ND11YLF-4412 920€


• Safety goggles (page 200) • Laser beam visualizer (page 199)• Nd:YAG crystal (page 130)


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Doping concentration 3-10 atm. %

Orientation [010]


Dimensional tolerancesDiameter: +0.00/-0.05 mm, Length: +0.00/-0.10 mm.







Nd:KGW LASER CRYSTALS

Nd:KGW crystals are low lasing threshold, highly efficient laser crystals perfectly suitable for laser range-finding applications. The efficiency of Nd:KGW lasers is 3 to 5 times higher than Nd:YAG lasers. Nd:KGW laser medium is one of the best choices ensuring effective laser generation at low pump energies (0.5 - 1 J ). These crystals feature high optical quality and great value of bulk resistance to laser radiation.


Description

Features

Miscellaneous

• Low lasing threshold• High bulk laser damage threshold• High efficiency• High optical quality• Diameter up to 12 mm and length up to 120 mm available on request



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Material Dimensions, mm Coatings Product ID Price

Nd(3%):KGW

3×3×2 AR/AR@1067&808 3-ND30KGW-10 390€3×3×3 AR/AR@1067&808 3-ND30KGW-11 390€3×3×4 AR/AR@1067&808 3-ND30KGW-12 390€3×3×5 AR/AR@1067&808 3-ND30KGW-13 390€Ø3×60 AR/AR@1067 3-ND30KGW-01 680€Ø4×80 AR/AR@1067 3-ND30KGW-02 760€Ø5×90 AR/AR@1067 3-ND30KGW-03 790€

Ø6×110 AR/AR@1067 3-ND30KGW-04 880€

Nd(5%):KGW

3×3×1 AR/AR@1067&808 3-ND50KGW-10 390€3×3×2 AR/AR@1067&808 3-ND50KGW-11 390€3×3×3 AR/AR@1067&808 3-ND50KGW-12 390€3×3×5 AR/AR@1067&808 3-ND50KGW-13 390€Ø3×60 AR/AR@1067 3-ND50KGW-01 680€Ø4×80 AR/AR@1067 3-ND50KGW-02 760€Ø5×90 AR/AR@1067 3-ND50KGW-03 790€

Ø6×110 AR/AR@1067 3-ND50KGW-04 880€

Catalog Items









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Material Yb:KGW/Yb:KYW

Doping concentration0.5-5 atm. % for Yb:KGW0.5-100 atm. % for Yb:KYW

OrientationB-cut: Nm-axis is parallel to input/output facesOther orientations svailable

Perpendicularity ±10 arcmin

Parallelism error ±5 arcsec




Yb:KGW AND Yb:KYW LASER CRYSTALS

Yb3+ doped KY( WO4)

2 (KYW ) and KGd( WO

4)

2 (KGW ) single crystals

are the new laser crystals for diode and laser pumped solid-state laser applications.Yb:KGW and Yb:KYW crystals are used as a lasing materials to generate ultrashort high power pulses. Yb:KGW can be used as ultrashort pulses amplifiers and these crystals are one of the best materials for high power thin disk lasers.The broad spectral emission band of Yb:KYW allows the tuning of the laser radiation over 1020-1060 nm range and the generation of femtosecond pulses shorter than 70 fs, enhanced storage capacity, wide absorption spectrum at 980 nm and high absorption of pump radiation in a small crystal region allows an efficient use of diode laser pump.As compared to YAG or glasses used as hosts for Yb3+, KYW and KGdW have the advantage of a larger absorption cross section than YAG, which decreases minimum pump intensity necessary to achieve transparency in the quasi-two-level system of ytterbium.


Description

Features

Miscellaneous

• High absorption coefficient @ 980 nm• High stimulated emission cross section• Low lasing threshold• Extremely low quantum defect• Broad output at 1020-1060 nm• High slope efficiency with diode pumping (>55%)• High Yb-doping concentration

• Custom design production is also available• Different doping levels available• Mass production at 2000 pieces per month available• Various end cuts available (plano/plano, wedge/wedge, brewster cut, etc.)• Various dielectric coatings are available.


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MaterialDimensions,

mmCoatings End surfaces Product ID Price

Yb(1%):KGW

5×5×2 AR/AR@980-1080 Right angle cut 3-YB1KGW-01 700€5×5×3 AR/AR@980-1080 Right angle cut 3-YB1KGW-02 700€5×5×5 AR/AR@980-1080 Right angle cut 3-YB1KGW-03 700€5×5×2 - Brewster angle cut 3-YB1KGW-04 740€5×5×3 - Brewster angle cut 3-YB1KGW-05 740€5×5×5 - Brewster angle cut 3-YB1KGW-06 740€

Yb(3%):KGW


Yb(5%):KGW


Yb(10%):KYW

5×5×1 AR/AR@980-1080 Right angle cut 3-YB10KYW-01 700€5×5×2 AR/AR@980-1080 Right angle cut 3-YB10KYW-02 700€5×5×3 AR/AR@980-1080 Right angle cut 3-YB10KYW-03 700€5×5×1 - Brewster angle cut 3-YB10KYW-04 740€5×5×2 - Brewster angle cut 3-YB10KYW-05 740€5×5×3 - Brewster angle cut 3-YB10KYW-06 740€

Yb(20%):KYW

5×5×1 AR/AR@980-1080 Right angle cut 3-YB20KYW-01 700€5×5×2 AR/AR@980-1080 Right angle cut 3-YB20KYW-02 700€5×5×3 AR/AR@980-1080 Right angle cut 3-YB20KYW-03 700€5×5×1 - Brewster angle cut 3-YB20KYW-04 740€5×5×2 - Brewster angle cut 3-YB20KYW-05 740€5×5×3 - Brewster angle cut 3-YB20KYW-06 740€

Catalog Items

• Laser beam visualizer (page 199)• Wavelength separators (page 60) • Laser crystal repolishing (page 261)



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Doping concentration 0.2-25 atm. %



Dimensional tolerancesDiameter: +0.00/-0.05 mm, Length: ±1 mm.






Yb:YAG LASER CRYSTALS

Ytterbium doped Yttrium Aluminum Garnet (Yb:YAG) crystal is one of the most promising laser-active materials.

It is more suitable for diode-pumping than the traditional Nd-doped systems. It can be pumped at 0.94 μm laser output. Compared with the commonly used Nd:YAG crystal, Yb:YAG crystal has a much larger absorption bandwidth to reduce thermal management requirements for diode lasers, a longer upper-state lifetime, three to four times lower thermal loading per unit pump power. Yb:YAG crystal is expected to replace Nd:YAG crystal for high power diode-pumped lasers and other potential applications.


Description

Features

Miscellaneous

• Ideal for diode pumping• Very low fractional heating, less than <11%• Very high slope efficiency, more than 56%• Broad absorption band, about 18 nm @ 940 nm• High thermal conductivity and strength

• Custom design production is also available• Mass production at 2000 pieces per month available• Various end cuts available (plano/plano, wedge/wedge, brewster cut, etc.)• Various dielectric coatings are available. Complex coatings are realized with IBS technique


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MaterialDimensions,

mmCoatings End surfaces Product ID Price

Yb(5%):YAG

5×5×2 AR/AR@940+1030 Right angle cut 3-YB05YAG-01 580€5×5×3 AR/AR@940+1030 Right angle cut 3-YB05YAG-02 580€5×5×5 AR/AR@940+1030 Right angle cut 3-YB05YAG-03 580€5×5×2 HR@1030+HT@940/AR@1030 Right angle cut 3-YB05YAG-04 650€5×5×3 HR@1030+HT@940/AR@1030 Right angle cut 3-YB05YAG-05 650€5×5×5 HR@1030+HT@940/AR@1030 Right angle cut 3-YB05YAG-06 650€5×5×2 - Brewster angle cut 3-YB05YAG-07 610€5×5×3 - Brewster angle cut 3-YB05YAG-08 610€5×5×5 - Brewster angle cut 3-YB05YAG-09 610€

Yb(10%):YAG

5×5×1 AR/AR@940+1030 Right angle cut 3-YB10YAG-01 580€5×5×2 AR/AR@940+1030 Right angle cut 3-YB10YAG-02 580€5×5×3 AR/AR@940+1030 Right angle cut 3-YB10YAG-03 580€5×5×1 HR@1030+HT@940/AR@1030 Right angle cut 3-YB10YAG-04 650€5×5×2 HR@1030+HT@940/AR@1030 Right angle cut 3-YB10YAG-05 650€5×5×3 HR@1030+HT@940/AR@1030 Right angle cut 3-YB10YAG-06 650€5×5×1 - Brewster angle cut 3-YB10YAG-07 610€5×5×2 - Brewster angle cut 3-YB10YAG-08 610€

5×5×3 - Brewster angle cut 3-YB10YAG-09 610€

Yb(20%):YAG

5×5×0,5 AR/AR@940+1030 Right angle cut 3-YB20YAG-01 580€5×5×1 AR/AR@940+1030 Right angle cut 3-YB20YAG-02 580€5×5×2 AR/AR@940+1030 Right angle cut 3-YB20YAG-03 580€

5×5×0,5 HR@1030+HT@940/AR@1030 Right angle cut 3-YB20YAG-04 650€5×5×1 HR@1030+HT@940/AR@1030 Right angle cut 3-YB20YAG-05 650€5×5×2 HR@1030+HT@940/AR@1030 Right angle cut 3-YB20YAG-06 650€5×5×1 - Brewster angle cut 3-YB20YAG-07 610€5×5×2 - Brewster angle cut 3-YB20YAG-08 610€5×5×3 - Brewster angle cut 3-YB20YAG-09 610€

Catalog Items





• Passive Q-switch crystals (page 140)


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• Passive Q-switch crystals (page 140)

Yb:CaF2 LASERCRYSTALS

Description

Due to Yb:CaF2 crystal low quantum defect and a comparably long fluorescence lifetime, ytterbium-doped gain media are preferably utilized for high-power diode-pumped systems and laser amplifiers with high optical-to-optical conversion efficiencies. From this point of view, Yb:YAG is now the most important and developed one. Just recently, ytterbium-doped alkaline-earth fluorides (Yb:CaF2) have attracted considerable interest for use in diode-pumped femtosecond (fs) lasers and amplifiers.Alkaline-earth fluorides which can be easily grown by using the standard Czochralski or Bridgman technique show a wide optical transmission range, a low dispersion behavior and limited nonlinear effects under intense laser irradiation. It was recently shown that Yb:CaF2 single crystal can be grown up to diameters of about 200 mm, which is superior for high-energy short-pulse lasers with centimeter-sized apertures.

Specifications Crystal structure Cubic

Point group m3m

Lattice parameters а = 5,462 Å,

Thermal expansion 18×10-6 /oC

Thermal conductivity 9.7 W/mK

Density 3,18 g/cm3

Mohs’ hardness 4

Melting temperature 1418o C

Refractive indices (l=1.06mm) no = 1,4

dn/dT -10,0×10-6 / оK

Fluorescence lifetime 2.4 ms

Emission cross section 2´10-21 cm2 @1030nm

Emission bandwidth 70 nm

Absorption cross section5.4 x 10-21 cm2 @980 nm

2.4 x 10-21 cm2 @923 nm

Catalog Items

Material Dimenssions, mm

Coating Product ID Price 1-3 pcs

Yb(3%):CaF2 6x6x5 AR/AR@1030 +940nm

3-YB03CAF-01 900€

Yb(5%):CaF2 6x6x5 AR/AR@1030 +940nm

3-YB05CAF-01 940€

Features

Miscellaneous

• Low quantum defect• Long fluorescence lifetime• Wide optical transmission range• Low dispersion behavior• Limited nonlinear effects under intense laser irradiation

• Custom design production is also available• Different doping levels available• Mass production at 2000 pieces per month available• Can be used to high-power diode-pumped systems and laser amplifiers• Various dielectric coatings are available.


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Absorption cross-section 5×10-18 cm2 @ 1064 nm


Dimensional tolerances +0.00/-0.2 mm






Cr4+:YAG CRYSTALS

Passive Q-switches or saturable absorbers provide high power laser pulses without electro-optic Q-switches, thereby reducing the package size and eliminating a high voltage power supply. ALTECHNA offers a wide range of solid state saturable absorbers such as Co:Spinel, Cr4+:YAG, V3+:YAG and others.

Cr4+:YAG is an excellent passive Q-switch crystal for Nd and Yb doped lasers (especially for Nd:YAG, Nd:YLF or Yb:YAG), if the wavelength is in the range of 900-1200 nm.


Description

Miscellaneous• Custom design production is also available• Different doping levels available• Mass production at 2000 pieces per month available• Various dielectric coatings are available. Complex coatings are realized with IBS technique• One of the best selling products in 2012!

Related products and accessories• Wavelength separators (page 60)


• Laser crystals (page 126)

• Laser crystal repolishing 261)• Optical coatings (page 86-98)


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Initial transmission @ 1064 nm Dimensions, mm Coatings Product IDPrice

*1-3pcs

T0=30%

Ø5 AR/AR@1064nm 3-CRYAG-30-05 230€3x3 AR/AR@1064nm 3-CRYAG-30-33 215€5x5 AR/AR@1064nm 3-CRYAG-30-55 230€

T0=40%


T0=50%


T0=60%


T0=70%


T0=80%


T0=85%


T0=90%


T0=95%


T0=97%


Catalog Items

Fill the Request Form at our Website to request Cr4+:YAG crystals with custom parameters!


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V3+:YAG CRYSTALS

V3+:YAG is a relatively new material for saturable absorber passive Q-switching in lasers emitting from 1.06 to 1.44 μm, in particular, for 1.3 um Nd-lasers.

Extremely high ground state absorption (GSA) cross section of 7x10-18 cm2 near 1.3 um and negligible excited state absorption (ESA) permits Q-switching of 1.3 and 1.44 um Nd-lasers without intracavity focusing both with flash-lamp and diode-laser pumping. Negligible excited-state absorption results in high contrast of Q-switch, i.e. the ratio of initial (small signal) to saturated absorption is higher than 10. Finally, excellent optical, mechanical, and thermal properties of the host crystal give an opportunity to design compact and reliable laser sources with this passive Q-switch crystal.


Description

Miscellaneous

• Custom design production is also available• Different doping levels available• Various dielectric coatings are available

Wavelength range 1000 - 1450 nm

Absorption cross-section 7.3×10-18 cm2 @ 1340 nm

Wavefront Distortion ≤λ/10 @ 632.8 nm

Dimensional Tolerances +0.00/-0.2 mm

Parallelism Error ≤20 arcsec


Surface Quality 10-5 Scratch & Dig


AR Coating Reflectivity ≤0.2% @ 1340 nm






• Laser crystal repolishing (page 261)• Optical coatings (page 86-98)


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Initial Transmission @ 1340 nmDimensions,

mmCoatings Product ID

Price*1-3pcs

T0=30%

Ø5 AR/AR @ 1340 nm 3-VYAG-30-05 610€3×3 AR/AR @ 1340 nm 3-VYAG-30-33 570€5×5 AR/AR @ 1340 nm 3-VYAG-30-55 610€

T0=40%

Ø5 AR/AR @ 1340 nm 3-VYAG-40-05 610€3×3 AR/AR @ 1340 nm 3-VYAG 40-33 570€5×5 AR/AR @ 1340 nm 3-VYAG-40-55 610€

T0=50%


T0=60%


T0=70%


T0=80%


T0=85%


T0=90%


T0=95%


T0=97%


Catalog Items


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Co:SPINEL (Co2+:MgAl2O

4)

CRYSTALS

Co2+:MgAl2O

4 (or Co:Spinel) is a relatively new material for

saturable absorber passive Q-switching in lasers emitting from 1.2 to 1.6 microns, in particular, for eye-safe 1.54 μm Er:glass laser.

High absorption cross section of 3.5 x 10-19 cm2 permits Q-switching of Er:glass laser without intracavity focusing both with flash lamp and diode-laser pumping. Negligible excited-state absorption results in high contrast of Q-switch, i.e. the ratio of initial (small signal) to saturated absorption is higher than 10. Finally, excellent optical, mechanical, and thermal properties of the crystal give an opportunity to design compact and reliable laser sources with this passive Q-switch.


Description Miscellaneous

• Custom design production is also available• Different doping levels available• Various dielectric coatings are available• Complex coatings are realized with IBS technique


Absorption cross-section 3.5×10-19 cm2 @ 1540 nm


Dimensional tolerances +0.00/-0.2 mm













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Initial transmission @ 1540 nmDimensions,

mmCoatings Product ID

Price*1-3 pcs

T0=30%

Ø5 AR/AR@1540 3-COSP-30-05 570€3x3 AR/AR@1540 3-COSP-30-33 490€5x5 AR/AR@1540 3-COSP-30-55 570€

T0=40%

Ø5 AR/AR@1540 3-COSP-40-05 570€3x3 AR/AR@1540 3-COSP 40-33 490€5x5 AR/AR@1540 3-COSP-40-55 570€

T0=50%


T0=60%


T0=70%


T0=80%


T0=85%


T0=90%


T0=95%


T0=97%


Catalog Items




NONLINEAR OPTICS

NONLINEAR CRYSTALS 147

•BBO crystals 147

•LBO crystals 149

•KTP crystals 151

•KDP, DKDP crystals 153

•LiNbO3 crystals 155

•AgGaSe2 crystals 156

•AgGaS2 crystals 156

•ZnGeP2 crystals 157

PHOTOREFRACTIVE CRYSTALS 158

•SBN crystals 158

•BSO crystals 160

•Fe:LiNbO3 crystals 162

RAMAN CRYSTALS 164

Please contact [email protected] if you are also interested in the following crystals:

LiIO3, KTA, CLBO

ZnGeP2, GaSe, CdGa

2S

4, LIS (LiInS

2), LiSe (LiInSe

2)

Visit www.altechna.com to see the latest news and regular updates.


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Beta Barium Borate BBO is a non-linear optical crystal that combines a number of unique features.

These features of nonlinear BBO crystal include wide transparency and phase matching ranges, large non-linear coefficient, high damage threshold and excellent optical homogeneity. Therefore, BBO provides an attractive solution for various non-linear optical applications like OPO, OPA, OPCPA and other. As a result of large thermal acceptance bandwidth, high damage threshold and small absorption BBO is well suited for frequency conversion of high peak or average power laser radiation. The large spectral transmission range as well as phase matching, especially in UV range, makes BBO perfectly suitable for frequency doubling of Dye, Argon and Copper vapour laser radiation, effective cascade harmonic generation (Frequency doublers, triplers, parametric amplifiers and wave mixers) of wide spread Nd:YAG as well as of Ti:Sapphire and Alexandrite laser radiation. Both angle tuned Type 1 (oo-e) and Type 2 (eo-e) phase matching can be obtained increasing the number of advantages for different applications.

Transparency range 189-3500 nm


Aperture tolerance +0.0/-0.1 mm

Orientation accuracy of cut angle <30 arcmin




Perpendicularity <5 arcmin

Material optical damage threshold >0.5 GW/cm2 for 10 ns pulses @ 1064 nm

BBO CRYSTALS

Description


Features

Miscellaneous

• Broad phase-matchable second-harmonic-generation (SHG) range from 409.6 nm to 3500 nm

• Wide transparency range from 189 nm to 3500 nm• Large effective SHG coefficient• High damage threshold of 10 GW/cm2 for 10 ns pulse-width at

1064 nm• Good mechanical and physical properties

• Custom design production is also available • Crystals with gold electrodes for electro-optical applications

available• AR, BBAR and PR coatings available• Crystal aperture up to 22x22 mm and length up to

20 mm available• Mass production capabilities: 1’000 pieces per month • Many BBO crystals are available from stock with fast delivery• IBS AR coatings for enhanced performance and longer lifetime

available


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BBO crystals for Ti:Sapphire lasersAperture

dimensions, mm

Length, mm Orientation θ/φ, degProtective coatings S1/S2,

nm/nmApplication Product ID

Price*1-3 pcs

6x6

0.1 29.2/90 400-800/400-800 SHG @ 800 nm 4-BBO-0601-0 455€0.1 44.3/90 400-800/266 THG @ 800 nm 4-BBO-0601-1 455€0.2 29.2/90 400-800/400-800 SHG @ 800 nm 4-BBO-0602-0 455€0.2 44.3/90 400-800/266 THG @ 800 nm 4-BBO-0602-1 455€0.5 29.2/90 400-800/400-800 SHG @ 800 nm 4-BBO-0605-0 360€0.5 44.3/90 400-800/266 THG @ 800 nm 4-BBO-0605-1 360€1 29.2/90 400-800/400-800 SHG @ 800 nm 4-BBO-0610-0 260€1 44.3/90 400-800/266 THG @ 800 nm 4-BBO-0610-1 260€2 29.2/90 400-800/400-800 SHG @ 800 nm 4-BBO-0620-0 260€

10x10

0.1 29.2/90 400-800/400-800 SHG @ 800 nm 4-BBO-1001-0 675€0.2 29.2/90 400-800/400-800 SHG @ 800 nm 4-BBO-1002-0 675€0.5 29.2/90 400-800/400-800 SHG @ 800 nm 4-BBO-1005-0 610€1 29.2/90 400-800/400-800 SHG @ 800 nm 4-BBO-1010-0 575€

BBO crystals for Yb:KGW/KYW lasersAperture

dimensions, mm

Length, mm Orientation θ/φ, deg AR coatings S1/S2, nm/nm Application Product IDPrice

*1-3 pcs

6x6

0.5 23.4/90 515+1030/515+1030 SHG @ 1030 nm 4-BBO-0605-2 490€1 23.4/90 515+1030/515+1030 SHG @ 1030 nm 4-BBO-0610-2 420€


8x8



10x10



12x12



20x20



All BBO crystals have type I (oo-e) phase matching. For more details contact [email protected]

Catalog Items


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Transparency range, nm 160-2800








Material optical damage threshold >10 GW/cm2 for 10 ns pulses @ 1064 nm

LBO CRYSTALS

Lithium Triborate LBOs high damage threshold, wide acceptance angle, good thermal stability and wide transmission range make it ideal for frequency doubling of high power lasers.

It is unique in many aspects, especially its wide transparency range, moderately high non-linear coupling, high damage threshold and good chemical and mechanical properties. Its transmission range is from 0.16 μm to 2.6 μm. LBO allows temperature-controllable non-critical phase-matching operation (NCPM) for 1.0-1.3 μm , Type I SHG, and also provides room temperature NCPM for Type II SHG at 0.8-1.1 μm. It possesses a relatively large angular acceptance bandwidth, reducing the beam quality requirements for source lasers.

Description


Features

Miscellaneous

• Broad transparency range from 160 nm to 2800 nm• Relatively large effective SHG coefficient (about three times

that of KDP)• High damage threshold (18.9 GW/cm2 for a 1.3 ns laser at

1053 nm)• Wide acceptance angle and small walk-off• Type I and Type II non-critical phase matching in a wide wave-

length range

• Apertures up to 40x40 mm and length up to 50 mm• Custom design production is also available• Mass production capabilities: 1’000 pieces per month • Many LBO crystals are available from stock with fast delivery• IBS AR coatings for enhanced performance and longer lifetime

available


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LBO crystals for Nd:YAG lasersAperture

dimensions, mm

Length, mm

Orientation θ/φ, deg

AR coatings S1/S2, nm/nm Application Product IDPrice

*1-3 pcs

3x3

10 42.2/90 1064+532/355THG @ 1064,Type II (e-oe)

4-LBO-3310-0 245€

10 90/11.6 1064+532/1064+532SHG @ 1064Type I (e-oo)

4-LBO-3310-1 245€

15 42.2/90 1064+532/355THG @ 1064Type II (e-oe)

4-LBO-3315-0 325€

15 90/11.6 1064+532/1064+532SHG @ 1064Type I (e-oo)

4-LBO-3315-1 325€

15 90/0 1064+532/1064+532SHG @ 1064NCPM I Type

4-LBO-3315-2 325€

20 90/0 1064+532/1064+532SHG @ 1064NCPM I Type

4-LBO-3320-0 405€

5x515 42.2/90 1064+532/355

THG @ 1064Type II (e-oe)

4-LBO-5515-0 765€

15 90/11.6 1064+532/1064+532SHG @ 1064Type I (e-oo)

4-LBO-5515-1 765€

LBO crystals for Yb:KGW/KYW lasersAperture

dimensions, mm

Length, mm Orientation θ/φ, deg AR coatings S1/S2, nm/nm Application Product IDPrice

*1-3 pcs

6x6

0.9 90/13.8 515+1030/515+1030 SHG @ 1030 nm 4-LBO-0609-2 490€1.9 90/13.8 515+1030/515+1030 SHG @ 1030 nm 4-LBO-0619-2 420€2.8 90/13.8 515+1030/515+1030 SHG @ 1030 nm 4-LBO-0628-2 465€3.7 90/13.8 515+1030/515+1030 SHG @ 1030 nm 4-LBO-0637-2 470€

8x8


10x10


12x12


20x20


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Aperture tolerances +0.0/-0.1 mm


Surface auality 10-5 Scratch & Dig




Material optical damage threshold >500 MW/cm2 for 10 ns pulses @ 1064 nm

KTP CRYSTALS

Single crystal Potassium Titanyl Phosphate is an excellent non-linear crystal. KTP is a standard crystal with the parameters mostly used in extracavity configuration when a single pass through the crystal is required.

It exhibits high optical quality, broad transparency range, relatively high effective SHG coefficient (about 3 times higher than that of KDP), rather high optical damage threshold, wide acceptance angle, small walk-off and Type I and Type II non-critical phase-matching (NCPM) in a wide wavelength range. KTP is the most commonly used material for frequency doubling of Nd:YAG lasers and other Nd-doped lasers, particularly at the low or medium power density range.

Description


Features

Miscellaneous

• Efficient frequency conversion and large non-linear optical co-efficients

• Wide transmission region from 350 nm to 4400 nm• Wide angular bandwidth and small walk-off angle• Broad temperature and spectral bandwidth• Low cost compared to BBO and LBO

• High grey track resistance (HGTR) KTP is available for high power applications

• Custom design production is also available• Mass production capabilities: 1’000 pieces per month • Many KTP crystals are available from stock with fast delivery




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Aperture dimensions,

mm

Length, mm

Orientation θ/φ, deg Coatings S1/S2, nm/nm Application Product IDPrice

*1-3 pcs

3x3 5 90/23.5 1064+532/1064+532 SHG@1064 4-KTP-3305 76€3x3 10 90/23.5 1064+532/1064+532 SHG@1064 4-KTP-3310 109€4x4 6 90/23.5 1064+532/1064+532 SHG@1064 4-KTP-4406 118€7x7 9 90/23.5 1064+532/1064+532 SHG@1064 4-KTP-7709 529€

Catalog Items

• 5APH59T-1 - adjustable polarizer / crystal holder (page 218)

• Special mount for crystals









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Aperture tolerances +0.0, 0.1






Material optical damage threshold >10 GW/cm2 (for KDP) >0.5 GW/cm2 (for DKDP) for 10 ns pulses @ 1064 nm

KDP, DKDP CRYSTALS

Nonlinear single crystals Pottasium Dideuterium Phosphate KDP and DKDP are widely used as the second, third and fourth harmonic generators for Nd:YAG and Nd:YLF lasers.

These crystals are also widely used for electro-optical applications as Q-switches for Nd:YAG, Nd:YLF, Ti:Sapphire and Alexandrite lasers, as well as for Pockels cells. The most commonly used electro-optical crystal is DKDP with a deuteration ratio more than 98%. These crystals are grown by a water-solution method and can be grown up to very large sizes. Therefore, they are available as low-cost and large-size finished non-linear components.

For frequency-doubling (SHG) and -tripling ( THG) of Nd:YAG laser at 1064 nm, both type I and type II phase-matchings can be employed with nonlinear single crystals KDP and DKDP. For frequency - quadrupling (FHG, output at 266 nm) of Nd:YAG laser KDP crystal is normally recommended.

Description


Features

Miscellaneous

• Good UV transmission• High optical damage threshold• High birefringence• High nonlinear coefficients • Negative thermal lensing

• Custom design production is also available • Mass production capabilities: 500 pieces per month • Many KDP crystals are available from stock with fast delivery• 400x400 mm aperture and 10- 50 mm length available• AR, BBAR and PR coatings available




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CrystalAperture x length,

mm

Orientation θ/φ, deg

AR coatings S1/S2, nm/nm Application Product IDPrice

*1-3 pcs

KDP 12x12x5 76.5/45 532+266/532+266 SHG@532nm, type I 4-KDP-1250-0 405€KDP 15x15x7 76.5/45 532+266/532+266 SHG@532nm, type I 4-KDP-1570-0 480€

DKDP 12x12x20 53.5/0 1064/1064+532 SHG@1064 nm, type II 4-DKD-1250-0 475€DKDP 12x12x20 59.3/0 1064+532/355 THG@1064 nm, type II 4-DKD-1250-1 475€DKDP 15x15x13 53.5/0 1064+532/1064+532 SHG@1064 nm, type II 4-DKD-1513-0 485€DKDP 15x15x13 36.5/45 1064+532/1064+532 SHG@1064 nm, type I 4-DKD-1513-1 485€DKDP 15x15x20 53.5/0 1064/1064+532 SHG@1064 nm, type II 4-DKD-1520-0 579€DKDP 15x15x20 59.3/0 1064+532/355 THG@1064 nm, type II 4-DKD-1520-1 579€

Catalog Items










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Aperture tolerances +0.0/-0.1 mm






Material optical damage threshold >250 MW/cm2

for 10 ns pulses @ 1064 nm

LiNbO3 CRYSTALS

Lithium Niobate is widely used as frequency doubling crystal for wavelengths over 1 micron and optical parametric oscillators (OPOs) pumped at 1064 nm as well as quasi-phase-matched (QPM) devices.

LiNbO3 is also one of the most attractive materials for

optoelectronics. A great variety of devices has been developed based upon this material.

ALTECHNA offers a lot of products made from high quality LiNbO

3 crystals of both acoustic and optical grades. Typically,

Czochralsky grown and poled along Z-axis boules are used with sizes up to 80 mm in diameter and 100 mm in length. Other boules orientations can be applied for some purposes (SAW substrates, piezotransducers).

Description


Features

Miscellaneous

• High homogeneity• Wide transparency range• Unique electro-optical, photoeleastic, piezoelectric and non-

linear properties• Good mechanical and chemical stability• Absorption loss < 0,1 %/cm @ 1064 nm

• LiNbO3 crystals with gold electrodes for electro-optic modula-

tors available• Fe, Zn, Gd, Cu, Y, B, Er doped LiNbO

3 crystals available

• AR and BBAR coatings available• We consult our customers to obtain optimal solution for the

various applications



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Transparency range0.9-16 µm (AgGaSe

2)

0.53-12 µm (AgGaS2)








Material optical damage threshold >350 MW/cm2 for 10 ns pulses @ 1064 nm

AgGaSe2, AgGaS

2 CRYSTALS

AgGaSe2 crystal has band edges at 0.73 and 18 µm. Its useful transmission range within 0.9–16 µm and wide phase matching capability provide excellent potential for OPO applications when pumped by a variety of currently available lasers. Tuning within 2.5–12 µm has been obtained when pumping by Ho:YLF laser at 2.05 µm; as well as non-critical phase matching (NCPM) operation within 1.9–5.5 µm when pumping at 1.4–1.55 µm. AgGaSe

2 has been demonstrated to be an efficient frequency

doubling crystal for infrared CO2 lasers radiation.

AgGaS2 crystal is transparent from 0.53 to 12 µm. Although its nonlinear optical coefficient is lower among the other IR crystals, high short wavelength transparency edging at 550 nm is used in OPOs pumped by Nd:YAG laser; in numerous difference frequency mixing experiments with diode, Ti:Sapphire, Nd:YAG and IR dye lasers covering 3–12µm range; in direct infrared countermeasure systems, and for SHG of CO2 laser. Thin AgGaS2 crystal plates are popular for ultrashort pulse generation in mid IR range by difference frequence generation employing NIR wavelength pulses.


Description

Features

• Large effective optical nonlinearity • Wide spectral and angular acceptances• Broad transparency range•High Figure of merit for non-linear interactions•Excelent crystal for three-wave interactions•Ultrashort pulse generation in mid IR range•Suitable for applications with CO

2 laser






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ZnGeP2 CRYSTALS

Zinc-Germanium Diphosphide (ZnGeP2, ZGP) single crystals

are highly-effective non-linear optical crystals for the mid-IR as well as terahertz range. ZnGeP

2 crystals have positive

birefringence which allows to carry out phasematched parametric frequency conversion of optical radiation in all the ranges of their background transparency spectrum from 0.75 to 12.0 µm. Its useful transmission range lies from 2.1 to 10.6 µm with absoprtion of lower than 0.04 cm-1. ZnGeP

2 has large

non-linear optical coefficient and a relatively high laser damage threshold.

Description

Applications:

Miscellaneous

• Second, third, and fourth harmonic generation of CO2 laser

• Optical parametric generation with pumping at a wavelength of 2.0 µm

• Second harmonic generation of CO-laser• Producing coherent radiation in sub-millimetre-range from

70.0 µm to 1000 µm - terahertz range• Generation of combined frequencies of CO

2 - and CO-lasers

radiation and other lasers are working in the crystal transpar-ency region

• High damage threshold AR coatings available• We consult our customers to obtain the optimal solution for IR

applications

Transparency range 0.75 – 12.0 µm




Surface quality 20-10 scratch-dig

Surface flatness <30 arcsec

Parallelism error <5 arcmin

Material optical damage threshold 60 MW/cm2 150 ns pulses @ 10.6 µm


* Contact ALTECHNA for pricing [email protected]

Transmission spectra of uncoated ZnGeP2 crystal, 14 mm thickness

General properties of ZnGeP2 crystals

Transparency range 0.75 - 12.0 µm

Point group 42 m

Density 4.12 g/cm3

Mohs hardness 5.5

Non-linear coefficientd36 = 68.9 pm/V (at 10.6 µm), d36 = 75.0 pm/V (at 9.6 µm)

Material optical damage threshold 60 MW/cm2 150 ns pulses @ 10.6 µm


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SBN CRYSTALS

Strontium-Barium Niobate is an excellent optical and photorefractive material.

Nominally pure and doped by Ce, Cr, Co, Fe SBN crystals of different compositions (SBN:61, SBN:75) are used in elecro-optics, acousto-optics, photorefractive non-linear optics. A new growing technique (Modified Stepanov technique) provides excellent optical quality single crystals, free of growth striations, inclusions and other inhomogeneities, as well as definite cross section and linear dimensions up to 100 mm. SBN crystalline elements meet the requirements for different applications. Based on this unique crystal growing technique, large high quality SBN optical elements and photorefractive cells are available.

Description

Standard dimensions (a x b x c)*, mm

Cerium doping, wt. %

CeO2

Product ID Price

5 x 5 x 5

undoped 4-SBN-0505-1 1140 €0.1 4-SBN-0505-2 1140 €

0.01 4-SBN-0505-3 1140 €0.002 4-SBN-0505-4 1140 €0.005 4-SBN-0505-5 1140 €

5 x 10 x 5

undoped 4-SBN-0510-1 2090 €0.1 4-SBN-0510-2 2090 €

0.01 4-SBN-0510-3 2090 €0.002 4-SBN-0510-4 2090 €0.005 4-SBN-0510-5 2090 €

5 x 15 x 5

undoped 4-SBN-0515-1 2660 €0.1 4-SBN-0515-2 2660 €

0.01 4-SBN-0515-3 2660 €0.002 4-SBN-0515-4 2660 €0.005 4-SBN-0515-5 2660 €

5 x 20 x 5

undoped 4-SBN-0520-1 3325 €0.1 4-SBN-0520-2 3325 €

0.01 4-SBN-0520-3 3325 €0.002 4-SBN-0520-4 3325 €0.005 4-SBN-0520-5 3325 €

Catalog Items

Features

Miscellaneous

• Very high quality crystals suitable for two- and four-wave mix-ing

• Perfect for electro-optical and acousto-optical applications• Suitable for pyroelectrical applications• Highly efficient phase conjugation

• Custom design production is also available • Other dopants: Ce, Cr, Co, Ni, La, Tm, Yb, Nd, Ce+La, are avail-

able.

* - c – along tetragonal axis

All standard crystals are poled and have carbon-water electrodes


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General properties of SBN crystals

SrxBa

1-xNb

2O

6

CompositionSBN:75 SBN:61

Melting point 1470-1490 оСMolecular weight 381.854 g-mol 388.813 g-molSymmetry 4 mmSpace group P4bmCell parameters a с

12.43024+/-0.00002 Ао

3.91341+/-0.00001 Ао

Formula units 5Density 5.4 g/cm3

Hardness 5.5Curie temperature 56 °С 80 °СRefractive index, (λ = 0,633 μm) n

o

ne

2.31172.2987

2.31032.2817

Δn, (λ = 0,633 μm) -0.0130 -0.0286

Transmission region 0.4 – 5.5 μm

Half-wave voltage Uλ/2

80 V 240 VElectrical conductivity 10-13 – 10-14 оhm-1 x cm-1

Dielectric constant, 20оС 340 900Electrooptical coefficient r

13

r33

r42

67 pm/V770 pm/V42 pm/V

47 pm/V250 pm/V

-Melting heat 120 2cal/gHeat capacity С

р0.12 kcal/g x К

Termoconductivity (1370-1470оС) 0.008 W/(cm x К)Pyroelectric coefficient, ν 0.28 μC x cm-2 x K-1 0.065 μC x cm-2 x K-1

Thermal expansion coefficient, α 10-6

α// а-axisα// с-axis

10 degree-1

9 (200-900oC) degree-1

• Laser beam visualizer (page 199) • Safety goggles (page 200)


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Transparency range 0.45 - 6 µm

Crystal symetry Cubic, 23

Orientation 110 cut, 100 cut

Density 9.20 g/cm2

Refractive index 2.54 at 0.633 µm

Mohs hardness 5

Melting point 900 deg

Electrooptical coefficient 5.0 (r41) pm/V at 0.633 µm

Dielectric constant (low frequency)

56

BSO CRYSTALS

Bismuth Silicon Oxide Bi12

SiO20

is a pale yellow, photoconductive electro-optic crystal which has found increasingly wide application.

The strong spectral dependence of the photoconductive properties of these crystals and their electrooptic properties makes it possible to develop a wide variety of devices including spatial light modulators, electrooptic sensors, hologram recording devices, phase conjugation, photorefractive incoherent-to-coherent optical converters, pockels readout optical memory (PROM), thin film optical waveguides, photorefraction.


Description

Features

Miscellaneous

• A wide variety of applications• High phase conjugation efficiency• Wide applications including pockels readout optical memory

(PROM), thin film optical waveguides, photorefraction and phase conjugation

• Not soluble in water or organic solvents

• Custom design production is available • Mass production available 500 pieces per month.


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Dimensions, mm Cut Coatings S1/S2* Electrodes Product ID Price

5x5x5 110 AR@532nm yes 4-BSO-0505-1 Call us

5x5x5 100 AR@532nm yes 4-BSO-0505-2 Call us5x5x7 110 AR@532nm yes 4-BSO-0505-3 Call us





10x10x10 100 AR@532nm yes 4-BSO-1010-4 Call us20x20x1 110 AR@532nm yes 4-BSO-2020-1 Call us


20x20x0.2 110 AR@532nm yes 4-BSO-2020-3 Call us

20x20x0.2 100 AR@532nm yes 4-BSO-2020-4 Call us

Catalog Items





* - Other wavelengths available on request.

• Laser beam visualizer (page 199) • Safety goggles (page 200)


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Transparency tange 0.35 – 5.5 µm

Crystal symetry Trigonal, 3m

Density 4.64 g/cm3

Mohs hardness 5

Melting point 1255

Refractive index at λ = 632.8 nm no = 2.29, n

e = 2.2

Electrooptical Coefficientλ = 632.8 nm

r33

= 32 pm/V at, r

22 = 6.8 pm/V at,

r31

= 10 pm/V at

Dielectric constant (low frequency)

ε11

= 85, ε33

= 30

Fe:LiNbO3 CRYSTALS

Lithium Niobate crystals doped with iron Fe:LiNbO3

are an excellent photorefractive material with high electro-optical coefficients and high photorefractive sensitivity and diffraction efficiency without an applied electric field. The crystals have wide applications in phase conjugation and holographic recording. ALTECHNA offers crystals with different Fe doping concentration, dimensions and optical processing requirements.


Description

Features

Miscellaneous

• A wide variety of applications, including optical laser device for writing a three dimensional hologram in the single crystal

• High phase conjugation efficiency• Multi-domain structure• High difraction efficiency

• Custom design production is also available • Custom dopant levels available• Mass production available 500 pieces per month


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Aperture, mm Thickness, mmDopant level, mol.

% Fe2O

3

Coatings S1/S2 Orientation Product ID Price

10x10 0.5

0.05* AR @ 532nm**90deg cut

(X-cut, Y-cut)***

4-FLN-1010-1 Call us10x10 1 4-FLN-1010-2 Call us10x10 5 4-FLN-1010-3 Call us10x10 10 4-FLN-1010-4 Call us20x20 0.5 4-FLN-2020-1 Call us

20x20 1 4-FLN-2020-2 Call us

Catalog Items

* - Dopant levels Fe2O

3 – 0.005% and 0.1% available. Call us.

** - Other wavelengths available. Call us.

*** - Z-cut and 45 deg cut available. Call us.

• 5APH59T-1 - adjustable polarizer / crystal holders (page 218)


• SBN crystals (page 158)







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Material Raman frequency shift, cm-1 Photon lifetime, psGain coeficient

at 1064 nm, cm/GW

CaCO3

1086.4 8.3 1.6

NaNO3

1069.2 10.0 7.0

Ba(NO3)

21048.6 25.0 10.0

KGd(WO4)

2901.0 and 768.0 1.9 and 1.6 3.8 and 4.4

KYb(WO4)

2908.6 and 757.0 1.4 and 0.7 3.6 and 3.8

KY(WO4)

2905.6 and 767.4 1.4 and 1.2 3.6 and 3.6

LiIO3

821.0 2.0 1.4

RAMAN CRYSTALS

Undoped Potassium Gadolinium Tungstate KGW, Potassium Yttrium Tungstate KYW and other Raman crystals for Raman conversion.ALTECHNA offers a large variety of nonlinear materials for high efficiency stimulated Raman scattering (SRS) conversion with low thresholds for nanosecond and picosecond laser pulses. These materials provide SRS conversion to a wide range of wavelengths.

To determine an output wavelength due to SRS the following formula is used:

Available crystals and crystal specifications

Description



LASERS AND LASER SYSTEMS

CW LASERS 166

•DL CW blue violet laser, 405 nm 166

•DPSS CW blue laser, 457 nm 167

•DPSS CW blue laser, 473 nm 168

•DPSS CW green laser, 532 nm 169

•DPSS CW yellow laser, 593.5 nm 170

•DPSS CW red laser, 671 nm 171

•DPSS CW IR laser, 1064 nm 172

•DL CW IR laser, 1550 nm 173

TINY DIODE LASER 174

EDUCATIONAL DPSS LASER KIT 175


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SpecificationsProduct ID

5-405-DL-0.03 5-405-DL-0.05 5-405-DL-0.1 5-405-DL-0.2 5-405-DL-0.03-LN 5-405-DL-0.05-LN 5-405-DL-0.1-LN

Output power, mW 30 50 100 200 30 50 100

Power stability, rms, over 4 hours

<5% <5% <5% <5% <1% <1% <1%

Transverse mode Near TEM00

Near TEM00

Near TEM00

Near TEM00

Near TEM00

Near TEM00

Near TEM00

M2 factor <1.5 <1.5 <1.5 <1.5 - - -

Beam divergence, mrad 0.5 0.5 0.5 0.5 0.5 0.5 0.5

Beam diameter at aperture, mm

~4.0 ~4.0 ~4.0 ~4.0 ~4.0 ~4.0 ~4.0

Warranty One year

Price 910€ 1190€ 1570€ 2930€ 1020€ 1350€ 1840€*- Power tunability is included option, that can be excluded for better price

*- TTL modulation is optional

*- Analog modulation is optional

*- RS232 interface is optional

*- Fiber coupling is optional

Catalog Items

DL CW BLUE vIOLET LASER, 405 nm

Applications

• DNA sequencing• Flow cytometry • Cell sorting• Optical instrument

• Spectrum analysis• Interference measurements• Holography • Laser lighting show

Description

The output power of 405-DPSS blue violet laser systems ranges from 1 mW to 300 mW. It is designed for easy operating and maintenance. 405nm blue laser Features: ultra compact, long lifetime, cost effective and easy operating. Different power stabilities (1%, 3%, 5%) available.

Wavelength 405 nm

Operating longitudinal mode Several

Polarization ratio >100:1

Point stability <0.05 mrad

Expected lifetime 10’000 hours

Standard specifications:

If you do not find suitable output power or other specifica-

tions do not meet you requirements please contact us and we

guaranty to provide a solution for you.


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5-457-DPSS-0.05 5-457-DPSS-0.1 5-457-DPSS-0.2 5-457-DPSS-0.55-457-DPSS-

0.05-LN5-457-DPSS-

0.1-LN5-457-DPSS-0.01-

SLM

Output power, mW 50 100 200 500 50 100 10


<5% <5% <5% <5% <1% <1% <1%


Near TEM00

Near TEM00

Near TEM00

Near TEM00

Near TEM00

Near TEM00

M2 factor <2.0 <2.0 <2.0 <3.0 <2.0 <2.0 <1.2

Beam divergence, mrad <1.5 <1.5 <1.5 <1.5 <1.5 <1.5 <1.2


~3.0 ~3.0 ~3.0 ~3.0 ~3.0 ~3.0 ~2.0

Noise of amplitude, rms < 30% < 30% < 30% < 30% < 3% < 3% < 0.5%

Warranty One year






Catalog Items

DPSS CW BLUE LASER, 457 nm

Applications


• Spectrum analysis• Interference measurements• Holography • Laser lighting show

Description

The output power of 457-DPSS blue laser systems ranges from 1 mW to 1 W. The laser system is TEC cooled. It is designed for easy operating and maintenance. 457nm blue laser Features: ultra compact, long lifetime, cost effective and easy operating. Different power stabilities (3%, 5%, 10%) available.

Wavelength 457 nm

Operating longitudinal mode Several / one (for SLM)









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0.03-LN5-473-DPSS-

0.05-LN5-473-DPSS-

0.02-SLM

Output power, mW 30 50 100 200 30 50 20


<5% <5% <5% <5% <1% <1% <1%

Transverse mode TEM00

TEM00

TEM00

TEM00

Near TEM00

Near TEM00

Near TEM00

M2 factor <1.2 <1.2 <1.2 <1.2 <1.2 <1.2 <1.2



~2.0 ~2.0 ~2.0 ~2.0 ~2.0 ~2.0 ~2.0

Noise of amplitude, rms < 30% < 30% < 30% < 30% < 1% < 1% < 0.5%

Warranty One year






Catalog Items

DPSS CW BLUE LASER, 473 nm

Applications


• Spectrum analysis• Interference measurements• Holography and etc.

Description

The output power of 473-DPSS blue laser systems ranges from 1 mW to 1 W. Laser system is TEC cooled. It is designed to be operated and maintained easily. 473nm blue laser is ultra compact, long lifetime, cost effective and easy operating. Different power stabilities (3%, 5%, 10%) available.

Wavelength 473 nm

Operating longitudinal mode Several / one (for SLM)









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0.1-LN5-532-DPSS-

0.5-LN5-532-DPSS-0.03-

SLM

Output power, mW 100 500 1000 5000 100 500 30


<10% <10% <10% <10% <1% <1% <1%

M2 factor <1.2 2.0 2.0 2.0 1.2 1.2 1.2


Near TEM00

Near TEM00

Near TEM00

Near TEM00

Near TEM00

TEM00



~2.0 ~3.0 ~3.0 ~3.0 ~2.0 ~2.0 ~2.0

Noise of amplitude, rms <5% <5% <5% <5% <1% <1% <0.5%

Warranty One year






Catalog Items

DPSS CW GREEN LASER, 532 nm

Applications

• Medical applications • Crystal inspections • Holography • Raman spectroscopy

Description

The output power of 532-DPSS green laser systems ranges from 10 mW to 5 W. Laser system is TEC cooled with high temperature stability. It is designed to be operated and maintained easily. Single longitudinal mode laser is available.

Wavelength 532 nm

Operating longitudinal mode

Several / one (for SLM)


Point stability <0.05







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5-593-DPSS-0.005 5-593-DPSS-0.01 5-593-DPSS-0.03 5-593-DPSS-0.05 5-593-DPSS-0.15-593-DPSS-

0.005-LN5-593-DPSS-

0.01-LN

Output power, mW 5 10 30 50 100 5 10


<5% <5% <5% <5% <5% <1% <1%

M2 factor <1.5 <1.5 <1.5 <1.5 <1.5 <1.5 <1.5



~2.0 ~2.0 ~2.0 ~3.0 ~3.0 ~2.0 ~2.0

Noise of amplitude, rms < 30% < 30% < 30% < 30% < 30% < 2% < 2%

Warranty One year

Price 3240€ 3960€ 5120€ 6020€ 8880€ 4550€ 5320*- Power tunability is included option, that can be excluded for better price





Catalog Items

DPSS CW YELLOW LASER, 593.5 nm

Applications

• Scientific experiment• Optical sensor• Measurement

• Communication• Spectrum analysis, etc.

Description

The output power of 593-DPSS Yellow Laser Systems ranges from 1 up to 500 mW. Laser system is TEC cooled. It is designed to be operated and maintained easily. Different power stabilities (3%, 5%, 10%) available.

Wavelength 593.5 nm

Operating longitudinal mode Several









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Wavelength 671 nm

Operating Longitudinal Mode

Several / one (for SLM)

Polarization Ratio >100:1

Point Stability <0.05

Expected Lifetime 10’000 hours

Catalog Items

DPSS CW RED LASER, 671 nm

Applications

• DNA sequencing • Flow cytometry• Cell sorting• Spectrum analysis• Interference

• Measurement • Holography• Laser printing • Chip inspection

Description

TEC cooled, high stability DPSS lasers, suitable for applications in harsh environments.ALTECHNA provides continuous wave 671-DPSS red laser system with wavelength of 671 nm, and the power range of 0.5 to 1 W. It is TEC cooled, high stability and suitable for applications in harsh environment. 671-DPSS laser system combines both high performance and budgetary price. Single longitudinal mode laser (spectral width <0.0001% and coherence length 50 m) is available.




0.1-LN5-671-DPSS-

0.2-LN5-671-DPSS-

0.5-LN5-671-DPSS-

0.02-SLM

Output power, mW 100 200 500 1000 100 200 500 20


<10% <10% <10% <10% <1% <% <1% <1%

M2 factor <1.2 <1.2 <1.2 <2.0 <1.2 <1.2 <1.2 <1.2

Beam divergence, mrad <1.5 <1.5 <1.5 <1.5 <2.0 <1.5 <1.5 <1.2


~2.0 ~2.0 ~2.0 ~2.0 ~2.0 ~2.0 ~2.0 ~2

Noise of amplitude, rms <30% <30% <30% <30% <1% <1% <1% <0.5%

Warranty One year

Price 980€ 1400€ 3440€ 4740€ 1540€ 1920€ 4350€ 5120€


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5-1064-DPSS-0.1

5-1064-DPSS-0.5

5-1064-DPSS-1.0

5-1064-DPSS-5.0

5-1064-DPSS-0.1-LN

5-1064-DPSS-0.5-LN

5-1064-DPSS-1.0-LN

5-1064-DPSS-0.5-SLM

Output power, mW 100 500 1000 5000 100 500 1000 500

Power stability <5% <5% <5% <5% <1% <1% <1% <1%


TEM00

TEM00

TEM00

TEM00

TEM00

TEM00

TEM00

M2 factor <1.5 <1.5 <1.5 <3.0 <1.5 <1.5 <1.5 <1.5



~2.0 ~2.0 ~2.0 ~3.0 ~2.0 ~2.0 ~2.0 ~2.0

Noise of amplitude, rms <5% <5% <5% <5% <1% <1% <1% <0.5%

Warranty One year

Price 660€ 1120€ 1840€ 7850€ 710€ 1250€ 1940€ 2380€*- Power tunability is included option, that can be excluded for better price





Catalog Items

DPSS CW IR LASER, 1064 nm

Applications

• Scientific experiment• Measurement• Optical instrument

• Optical sensor• Communication• Spectrum analysis

Description

DPSS-IR lasers are suitable for applications in harsh or industrial environments, requiring no additional heat sinking. DPSS-IR laser system combines both high performance and affordability with an emphasis on satisfying a variety of applications as budgetary needs. Power levels range from 50 mW to 10 W.

Wavelength 1064 nm

Polarization ratio > 100:1


Expected lifetime > 10'000 hours






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5-1550-DL-0.1 5-1550-DL-0.2 5-1550-DL-0.5 5-1550-DL-1.0 5-1550-DL-2.05-1550-DL-

0.1-LN5-1550-DL-

0.2-LN5-1550-DL-

0.5-LN

Output power, mW 100 200 500 1000 2000 100 200 500

Power stability <5% <5% <5% <5% <5% <1% <1% <1%


Near TEM00

Near TEM00

Near TEM00

Near TEM00

Near TEM00

Near TEM00

Near TEM00

M2 factor <20 <20 <20 <20 <20 <20 <20 <20



~5×8 ~5×8 ~5×8 ~5×8 ~5×8 ~5×8 ~5×8 ~5×8

Noise of amplitude, rms <30% <30% <30% <30% <30% <1% <1% <1%

Warranty One year

Price 2520€ 2970€ 4040€ 5510€ 5960€ 2960€ 3450€ 4610€*- Power tunability is included option, that can be excluded for better price





Catalog Items

DL CW IR LASER, 1550 nm

Applications

• Scientific experiment• Measurement• Optical instrument

• Optical sensor• Communication• Spectrum analysis

Description

Diode infrared lasers at 1550nm are used in measurement, communication, spectroscopy, and medical applications. The wavelength is in “eye-safe” spectrum region which makes the laser far less dangerous than e.g. 1-μm lasers with similar output powers. Diode laser at 1550 can be used as budgetary substitute for Erbium lasers. Power levels range from 50 mW to 3 W.

Wavelength 1550 nm

Polarization ratio > 50:1


Expected lifetime > 10'000 hours






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TINY DIODE LASER

Catalog items:

Description:

Tiny diode laser is a precisely controlled light source. It consists of laser diode which is built in custom temperature controlled diode laser driver. This driver has all the specifications of TINY LDD. Diode laser fiber is covered with metal shield. We offer standard wavelength and power diode lasers. However, we can put any diode compatible with TINY LDD in this system.


Features:

• Soft start function• TEC controller• Overheating protection• Stand alone and USB 2.0 compatible • Metal shielded fiber• Compact size• Smooth temperature stabilization• Ready-to-use pumping solution• 1 year warranty• Custom modifications available

Wavelength, nm Diode power, W Diode core diameter, µm/NA Product ID Price

808 4 105/0.15 TDL-808 2200€

915 9 105/0.15 TDL-915 2300€

940 9 105/0.15 TDL-940 2300€

975 9 105/0.15 TDL-975 2300€

1064 7 105/0.15 TDL-1064 2300€

Wavelength 808, 915, 940, 975, 1064 nm

Numerical aperture (NA) 0.15

Spectral width (FWHM) 3 nm

Power conversion efficiency 50 %

Adjustable current range 0.4 – 10 A (0.004 A per step)

voltage limitation range 1.5 – 3 v (0.001 v per step)

Bipolar TEC controller current ± 4 A

External power supply2 x 100 – 240 v AC + 5 v 8 A DC

Temperature control range 10 – 45°C (0.1°C per step)

Multi-mode fiber 105 µm

Size (without stop button and key) 180 x 120 x 45mm

Fiber length 1 m

Connector FC fiber-optic

Operates in CW


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EDUCATIONAL DPSS LASER KITDescription

We offer new DPSS laser educational kit for students and scientists. The product itself is designed for wide range of users and education topics. This kit is perfect for students who need to understand the basics of laser performance. We have developed three basic versions of the product: one operates in CW, the other is an upgrade with QCW operation mode and the last one can generate 2nd harmonic. We encourage you to build your own kit! Tell us what you need and we will create a kit designed just for your lab and education program.

Features

• Easy and understandable system for educational purposes;• compact micro laser;• possible to change combination of the crystals;• laser diode temperature control;• laser for cavity adjustment;• dust secured fiber;• easy to adjust some of the stages and holders;• only 62 mm beam elevation from the breadboard;• possibility to generate second harmonic (Pro kit version);• variable resonator length.

DPSS laser educational kit

Specifications

• CW or CW/QCW mode (optional);• pro Kit version generates the 2nd harmonic;• up to 10 W diode power;• Yb (Yb=10%): YAG L=2 mm, max CW power 2 W (can be limited);• up to 11 kHz frequency in QCW;• possible wavelengths: Yb:YAG 1030nm, Nd:YAG 1064nm;• beam quality : ~M2 < 1.2 with Yb:YAG;• positioned on 1,5 cm high, 30 cm wide and 40 cm long breadboard.

Enhanced DPSS Kit

Fiber

Cr:YAG

Laser diode driver TINY LDD

Focus lenseVisualizator

Yb:YAG Resonator

Laser diode

Basic structure of Enhanced DPSS Laser Kit

Basic DPSS laser Kit Enhanced DPSS laser Kit Pro DPSS laser Kit•LaserdiodedriverTinyLDD;•anylaserdiodebyyourchoicecom-

patible with Tiny LDD (up to 10 W);•filters (Notch, pumping/generation

avoidance etc.);•focusinglens;•Yb:YAG;•resonatormirrors;•visualizer;•variousholdersandstages;•laserforcavityadjustment.

•LaserdiodedriverTinyLDD;•anylaserdiodebyyourchoicecom-

patible with Tiny LDD (up to 12 W);•filters (Notch,pumping/generation

avoidance etc.);•focusinglens;•Yb:YAGandCr:YAGcrystals;•resonatormirrors;•visualizer;•variousholdersandstages;•laserforcavityadjustment.

•LaserdiodedriverTinyLDD;•anylaserdiodebyyourchoicecompatiblewithTinyLDD(upto12W);•filters(Notch,pumping/generationavoidanceetc.);•focusinglens;•Yb:YAGcrystal;•Cr:YAGcrystal;•KTPnonlinearcrystal;•resonatormirrors;•visualizer;•variousholders,rotationstages,smallbreadboard;•additionallenses;•laserforcavityadjustment.

Operates in CW Operates in CW/QCW Generates 2nd harmonic5000€ 6000€ 7500€

* Custom versions available

LASER ACCESSORIES AND EQUIPMENT

WATT PILOT 177

•Standard Watt Pilot 177

•Enhanced Watt Pilot 179

•Ultrafast Watt Pilot 181

•Motorized Watt Pilot 183

LASER ACCESSORIES AND EQUIPMENT 186

•Beam expanders 186

•Motex - motorized tunable beam expander 188

•Laser beam shaping systems 189

•Autocorrelators 192

•High speed photodetectors 194

•High power laser shutters 196

•Beam dumps 197

• IR viewer 198

•Laser Visualizers 199

•Spectacles and goggle type safety Gglasses 200

•Laser diodes and modules 203

•Optical chopper 204


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Antireflection coating R < 0.25% all entrance and exit surfaces

Attenuation range 0,5 - 95% for transmitted p-pol beam

Extinction ratio Ts/T

p<1:500

Type of configuration Medium power Medium power enhanced performance High power

Clear aperture 15 mm (up to 50 mm are available) 15 mm (up to 50 mm are available) 10 mm (up to 50 mm are available)

Configurationλ/2 low order waveplate + polarizing

cubeλ/2 zero order waveplate + cemented

polarizing cubeλ/2 zero order waveplate + optically con-

tacted polarizing cube

Operational wavelength range ±2 nm ±10 nm ±10 nm

Damage threshold >0,3 J/cm2 for 10 ns 10Hz pulses at 1064 nm, typical >20 J/cm2 for 10 ns 10Hz pulses at 1064 nm

STANDARD WATT PILOT

Continuously variable attenuator/beamsplitter for down to 350 fs laser pulses.

Variable attenuator/beamsplitter consists of 2 high-performance polarizing optics components placed in precision opto-mechanical holder 5APH79T-1. Variable attenuator/beamsplitter incorporates a high-performance Polarizing Cube Beamsplitter which reflects s-polarized light while transmitting p-polarized light. A rotating quartz Phase λ/2 Waveplate is placed in the incident polarized laser beam. The intensity ratio of those two beams may be continuously varied without alteration of other beam parameters by rotating the waveplate. Ratio can be controlled over a wide dynamic range. Pure p-polarization could be selected for maximum transmission, or pure s-polarization for maximum attenuation of the transmitted beam.

Description


Features

• Divides laser beam into two beams of manually adjustable intensity ratio

• Convenient 90 deg angle between reflected and transmitted beams

• Negligible beam deviation

Miscellaneous

• Originally developed and manufactured at ALTECHNA• One of the best selling product in 2012!• Short delivery (1-2 weeks) for most of the standard

models

Every Watt Pilot model can be upgraded to motorized version for additional 750€


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Wavelength,nm

Clear aperture, mm

Medium power (with cemented polarizing cube)

Medium power enhanced performance (with cemented polarizing cube)

Product ID Price Product ID Price532 15 2-CVB-MP-15-0532 600€ 2-CVB-MPEP-15-0532 640€633 15 2-CVB-MP-15-0633 600€ 2-CVB-MPEP-15-0633 640€

780 15 2-CVB-MP-15-0780 600€ 2-CVB-MPEP-15-0780 640€

850 15 2-CVB-MP-15-0850 600€ 2-CVB-MPEP-15-0850 640€1064 15 2-CVB-MP-15-1064 600€ 2-CVB-MPEP-15-1064 640€1310 15 2-CVB-MP-15-1310 600€ 2-CVB-MPEP-15-1310 640€1550 15 2-CVB-MP-15-1550 600€ 2-CVB-MPEP-15-1550 640€

Catalog Items


• Motorized Watt Pilot (page 183)

• Beam dump 10BD (page 197)


*Motorized Standard Watt Pilot version cost 750€ extra.

Wavelength,nm

Clear aperture, mm

High power (with optically contacted polarizing cube)

Product ID Price355 10 2-CVB-EPOC-10-0355 860€532 10 2-CVB-EPOC-10-0532 810€633 10 2-CVB-EPOC-10-0633 810€780 10 2-CVB-EPOC-10-0780 810€850 10 2-CVB-EPOC-10-0850 810€

1064 10 2-CVB-EPOC-10-1064 810€1310 10 2-CVB-EPOC-10-1310 810€1550 10 2-CVB-EPOC-10-1550 810€

Motorized version of Standard Watt Pilot - page 183


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Clear aperture Standard 15 mm (up to 50 mm are available)

Time dispersion t < 4 fs for 100 fs Ti:Sapphire laser pulses

Optimization Reflection mode Broad-band reflection mode Transmission mode

Configurationλ/2 ZeroOrder waveplate + 2x Brewster

type thin film polarizersλ/2 ZeroOrder waveplate + 2x Broadband

Brewster type thin film polarizersλ/2 ZeroOrder waveplate + 1x Brewster

type thin film polarizer

Operational wavelength range ±5 nm ±20 nm ±5 nm

Attenuation range @ CWL 0.3 - 99 % for reflected s-pol beam 0.5 - 98 % for reflected s-pol beam 0.3 - 95 % for transmitted p-pol beam

Damage threshold >5 J/cm2; >100 mJ/cm2 @ 100 fs 10Hz, 800 nm

ENHANCED WATT PILOT

Enhanced Watt Pilot series devices consists of a rotating phase retardation λ/2 waveplate and Brewster type thin film polarizers which both are placed in precision opto-mechanical holder. The intensity of the laser beam can be manually controlled over a wide dynamic range.

To serve most of the existing laser sources ALTECHNA developed several models of Watt Pilot.

Quick selection guide will help you to choose the most suitable model for your laser.

Description


Features

• Divides laser beam into several beams of manually adjustable intensity ratio

• Ideal for femtosecond and high energy laser applications• High optical damage threshold

Miscellaneous

• Originally developed and manufactured at ALTECHNA • One of the Best Selling Product in 2012!• Short delivery (1-2 weeks) for most of the standard models



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Mode λ, nm

Reflection mode Broad-band Reflection mode Transmission mode

Product ID Price Product ID Price Product ID Price

266 2-EWP-R-0266 750€ n/a 2-EWP-T-0266 730€

355 2-EWP-R-0355 720€ n/a 2-EWP-T-0355 700€

400 2-EWP-R-0400 720€ n/a 2-EWP-T-0400 700€515 2-EWP-R-0515 720€ n/a 2-EWP-T-0515 700€

532 2-EWP-R-0532 720€ n/a 2-EWP-T-0532 700€

780 2-EWP-R-0780 720€ n/a 2-EWP-T-0780 700€780-820 n/a 2-EWP- BBR-0800 820€ 2-EWP-T-7882 740€

800 2-EWP-R-0800 720€ n/a 2-EWP-T-0800 700€1020-1040 n/a 2-EWP- BBR-1030 820€ 2-EWP-T-1030 740€

1064 2-EWP-R-1064 720€ n/a 2-EWP-T-1064 700€1550 2-EWP-R-1550 720€ n/a 2-EWP-T-1550 700€

Catalog Items

• Motorized Watt Pilot (page 183)

• Beam dump 10BD (page 197)


*Motorized Watt Pilot version cost 750€ extra.

Motorized version of Enhanced Watt Pilot - page 183


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Standard CWL 800 nm or 1030 nm (other available upon request)

Clear aperture Standard 15 mm (up to 50 mm available)

Wavelength range +/-25 nm @ CWL +/-50 nm @ CWL

Configurationλ/2 zero order waveplate +

2x broadband (ultraFAST) thin film polarizersλ/2 achromatic waveplate +

2x broadband (ultraFAST) thin film polarizers

OptimizationTransmission

mode Transmission

contrast modeReflection

mode Reflection

Contrast modeTransmission

modeTransmission contrast mode

Reflection mode

Reflection Contrast mode

Attenuation range @ CWL Tp ~ 1 - 85 % Tp ~ 0.2 - 70 % Rs ~ 4 - 96 % Rs ~ 0.1 - 70 % Tp ~ 1 - 85 % Tp ~ 0.2 - 70 % Rs ~ 4 - 96 % Rs ~ 0.1 - 70 %

Damage threshold>5 J/cm2 10 ns 10 Hz pulses @ 1064 nm;

>100 mJ/cm2 @ 100 fs 10 Hz, 800 nm

ULTRAFAST WATT PILOT

Ideal for ultraSHORT laser pulses (down to 20 fs)

Variable attenuator consists of zero order (air-spaced) λ/2 quartz waveplate and two (or one) high-performance broadband 72 degree polarizers. Rotating waveplate changes ratio of s and p polarizations. Polarizers working at 72 deg angle of incidence (AOI) reflect s-polarized light while transmitting p-polarized light. Intensity ratio of those two beams can be continuously varied without alteration of other beam parameters by rotating the waveplate. Intensity of either exit beams can be controlled over a wide dynamic range. P-polarization could be selected for maximum transmission, or high-purity s-polarization could be reflected when maximum attenuation of the transmitted beam takes place.

There are 4 types of UltraFAST attenuators: they can be reflection or transmission type and contrast or transmission/reflection optimized. For more information and curves on polarizers please check broadband (ultrafast) thin film polarizers section (page 107).

Description


Features• Ideal for ultra SHORT femtosecond lasers • Divides laser beam into two beams of manually adjustable

intensity ratio • High optical damage threshold • Low dispersion for femtosecond laser pulses



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Miscellaneous

• Originally developed and manufactured at ALTECHNA • One of the Best Selling Product in 2012!• Short delivery (1-2weeks) for most of the standard models


λ/2 zero order waveplate + 2x broadband (ultraFAST) thin film polarizers

Transmission modeTransmission

contrast modeReflection mode

Reflection contrast mode

775 - 825 2-UWP-T1-0800 2-UWP-T2-0800 2-UWP-R1-0800 2-UWP-R2-0800Price 1220€ 1220€ 1220€ 1220€

1005 - 1055 2-UWP-T1-1030 2-UWP-T2-1030 2-UWP-R1-1030 2-UWP-R2-1030Price 1220€ 1220€ 1220€ 1220€

Catalog Items

• Yb:KGW and Yb:KYW crystals (page 135)• Autocorrelator (page 192)• Beam dump 10BD (page 197)



λ/2 achromatic waveplate + 2x broadband (ultraFAST) thin film polarizers

Transmission modeTransmission

contrast modeReflection mode

Reflection contrast mode

750-850 2-UWPA-T1-0800 2-UWPA-T2-0800 2-UWPA-R1-0800 2-UWPA-R2-0800Price 1380€ 1380€ 1380€ 1380€

980-1090 2-UWPA-T1-1030 2-UWPA-T2-1030 2-UWPA-R1-1030 2-UWPA-R2-1030Price 1380€ 1380€ 1380€ 1380€

*Motorized Watt Pilot version cost 750€ extra.

Motorized version of UltraFAST Watt Pilot - page 183

Large aperture Watt Pilot, CA=Ø40mm


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Clear aperture Standard 15mm (up to 50mm are available)

Dimensions91x63x118 mm (For Standard and Enhanced) 91x63x107mm (For UltraFAST)

Number of steps in full rotation (360°) 31 200, one step corresponds to 41.54 arc sec

Rotation speed at 1000 steps per second 11.54 deg/s

Step accuracy in full rotation ±10 steps*

Backlash ±10 steps

Mechanical Specifications

Features

• User-friendly software interface• High rotation step resolution (0,4 mrad/step)•Negligible beam deviation•Stand-alone USB powered controller•Easy to integrate

MOTORIZED WATT PILOT

Motorized Watt Pilot is a computer controlled laser beam attenuator. It attenuates free space laser beam/pulse continuosly without introducing additional energy fluctuations. Watt Pilot is essential in systems, where stable laser power adjusting is necessary. Despite stand alone device look, Motorized Watt Pilot is very compact and it can be easily integrated in custom optical system.

Description

• Beam dump 10BD (page 197) • Visualisers (page 199)


* Step accuracy for single start/stop rotation (not full cycle) depends on acceleration and speed of stepper motor; these parameters are user-controlled.

Miscellaneous

• Originally developed and manufactured at ALTECHNA • One of the Best Selling Product in 2012!• Short delivery (1-2 weeks) for most of the standard models



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Step 1 Place polarizers into mechanical adapter. Polarizers must face each other with surfaces coated with polarizing coating. Polarizing coating is marked with an arrow, so you have to put the polarizers with the arrows on the sides facing each other. Then fix polarizers with the plastic bolts (use all 4 plastic bolts to fix one polarizer).

NOTICE: do not tighten up the bolts too much since it can bend the polarizer and thus distort the laser beam.

Step 2 Put wave plate into attenuator between two mounting rings as shown. Be sure the wave plate is immobilized tightly.

Step 3 Attenuator consists of two mechanical parts. You should assemble both mechanical parts together.

Step 4 Use fixing screw for tightening both parts together.

Motorized Watt Pilot assembling steps

ModelClear

aperture, mm

Operational wavelength range, nm

Configuration OptimizationAttenuation range@CWL

Damage threshold@10ns, 1064nm, 10Hz

Product ID Price

Standard

15

532

λ/2 LowOrder waveplate + cemented

polarizing cube

Transmission/reflection mode

0.5-95% for transmitted p-pol beam

>0.3J/cm2

2-CVB-MP-15-0532-M 1350€633 2-CVB-MP-15-0633-M 1350€780 2-CVB-MP-15-0780-M 1350€850 2-CVB-MP-15-0850-M 1350€

1064 2-CVB-MP-15-1064-M 1350€1310 2-CVB-MP-15-1310-M 1350€1550 2-CVB-MP-15-1550-M 1350€

15

532

λ/2 ZeroOrder waveplate + cemented

polarizing cube

>0.3J/cm2

2-CVB-MPEP-15-0532-M 1390€633 2-CVB-MPEP-15-0633-M 1390€780 2-CVB-MPEP-15-0780-M 1390€850 2-CVB-MPEP-15-0850-M 1390€

1064 2-CVB-MPEP-15-1064-M 1390€1310 2-CVB-MPEP-15-1310-M 1390€1550 2-CVB-MPEP-15-1550-M 1390€

10

532

λ/2 ZeroOrder waveplate +

optically contacted

polarizing cube

>20J/cm2

2-CVB-EPOC-10-0532-M 1560€633 2-CVB-EPOC-10-0633-M 1560€780 2-CVB-EPOC-10-0780-M 1560€850 2-CVB-EPOC-10-0850-M 1560€

1064 2-CVB-EPOC-10-1064-M 1560€1310 2-CVB-EPOC-10-1310-M 1560€1550 2-CVB-EPOC-10-1550-M 1560€

Catalog Items


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ModelClear

aperture, mm

Operational wavelength range, nm

Configuration OptimizationAttenuation range@

CWL

Damage threshold@10ns, 1064nm, 10Hz

Product ID Price

Enhaced 15

266

λ/2 ZeroOrder wave-plate +

2X Brewster type thin film polarizers

Reflection0.3-99% for reflected

s-pol beam

>5J/cm2

>100mJ/cm2 @100fs, 800nm

2-EWP-R-0266-M 1500€355 2-EWP-R-0355-M 1470€400 2-EWP-R-0400-M 1470€515 2-EWP-R-0515-M 1470€532 2-EWP-R-0532-M 1470€780 2-EWP-R-0780-M 1470€800 2-EWP-R-0800-M 1470€

1064 2-EWP-R-1064-M 1470€

1550 2-EWP-R-1550-M 1470€

780-820 λ/2 ZeroOrder wave-plate + 2X broadband

Brewster type thin film polarizers

Broadband re-flection mode

0.5-98% for reflected s-pol beam

2-EWP-BBR-0800-M 1570€

1020-1040 2-EWP-BBR-1030-M 1570€

266


1X Brewster type thin film polarizers

Transmission mode

0.5-95% for transmit-ted p-pol beam

2-EWP-T-0266-M 1480€355 2-EWP-T-0355-M 1450€400 2-EWP-T-0400-M 1450€515 2-EWP-T-0515-M 1450€532 2-EWP-T-0532-M 1450€780 2-EWP-T-0780-M 1450€

780-820 2-EWP-T-7882-M 1490€800 2-EWP-T-0800-M 1450€

1020-1040 2-EWP-T-1030-M 1490€1064 2-EWP-T-1064-M 1450€1550 2-EWP-T-1550-M 1450€

UltraFAST 15

775-825


2X broadband (Ultra-FAST)


Transmission mode

1-85% for transmit-ted p-pol beam

>5J/cm2

>100mJ/cm2 @100fs, 800nm

2-UWP-T1-800 1970€1005-1055 2-UWP-T1-1030 1970€

775-825 Transmission contrast mode

0.2-7% for transmit-ted p-pol beam

2-UWP-T2-800 1970€1005-1055 2-UWP-T2-1030 1970€

775-825 Reflection mode

4-96% for reflected s-pol beam

2-UWP-R1-800 1970€1005-1055 2-UWP-R1-1030 1970€

775-825 Reflection contrast mode


2-UWP-R2-800 1970€

1005-1055 2-UWP-R2-1030 1970€

750-850

λ/2 achromatic wave-plate +

2X broadband (Ultra-FAST)


Transmission mode

1-85% for transmit-ted p-pol beam

2-UWPA-T1-800 2130€980-1090 2-UWPA-T1-1030 2130€750-850 Transmission

contrast mode0.2-7% for transmit-

ted p-pol beam2-UWPA-T2-800 2130€

980-1090 2-UWPA-T2-1030 2130€750-850 Reflection

mode4-96% for reflected

s-pol beam

2-UWPA-R1-800 2130€

980-1090 2-UWPA-R1-1030 2130€

750-850 Reflection contrast mode


2-UWPA-R2-800 2130€980-1090 2-UWPA-R2-1030 2130€


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Lens material BK7, FS, UVFS

Wavelength 355, 532, 1064 nm or by request

Housing material Black or white anodized aluminium

Transmited wavefront disortion λ/4 p-v at 633 nm over clear aperture

Transmission >97%


Miscellaneous


• Custom design beam expanders are available in small and mass production quantities

• Fill the request form at our website to request beam expander

• Laser beam shaping systems (page 190)

BEAM EXPANDERS

The most common type of beam expander is derived from the Galilean telescope which usually has one negative input lens and one positive output lens. For low expansion ratios (1.3 - 20 times) the Galilean telescope is most often employed due to its simplicity, small package size and low cost.

We offer beam expander made from two, three, or more spherical lens made from BK7, FS, UVFS or other glass.

Description

Tunable 2x - 8x laser beam expander

Tunable 2x - 8x dual wavelength laser beam expander

Beam expanders for scientific and industrial applications!

Beam expander


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Fixed ratio beam expanders

Expansion ratio Wavelength, nm Input aperture, mm Exit aperture, mm Product ID Price

2X 1064 >5 25 6-BE-2X-1064 245€

3X 1064 >5 25 6-BE-3X-1064 245€

4X 1064 >5 25 6-BE-4X-1064 245€

5X 1064 >3 18 6-BE-5X-1064 254€

6X 1064 >3 18 6-BE-6X-1064 254€

8X 1064 >3 18 6-BE-8X-1064 266€

10X 1064 >3 18 6-BE-10X-1064 270€

12X 1064 >3 18 6-BE-12X-1064 270€

2X 532 >5 25 6-BE-2X-532 265€

3X 532 >5 25 6-BE-3X-532 265€

5X 532 >3 18 6-BE-5X-532 274€

10X 532 >3 18 6-BE-10X-532 290€

2X 355 >5 25 6-BE-2X-355 298€

3x 355 >5 25 6-BE-3X-355 298€

5X 355 >3 18 6-BE-5X-355 305€

10X 355 >3 25 6-BE-10X-355 324€

Tunable laser beam expander

Expansion Ratio Wavelength, nmInput Aperture,

mmExit Aperture,

mmHousing Diameter,

mmHousing Length,

mmProduct ID Price

Tunable 2X - 8X 1064 4.5 - 11 36 45 - 50 114 - 142 6-BE-MA-1064 960€

Tunable 2X - 8X 532 4.5 - 11 36 45 - 50 114 - 142 6-BE-MA-532 980€

Tunable 2X - 11X 355 4.5 - 11 36 45 - 50 112 - 142 6-BE-MA-355 1290€

Tunable dual wavelength laser beam expander

Expansion ratio Wavelength, nmInput aperture,

mmExit aperture,

mmHousing diameter,

mmHousing length,

mmProduct ID Price

Tunable 2X - 8X 1030 / 515 4.5 - 11 36 45 - 50 114 - 142 6-BE-T-1030-515 1450€

Tunable 2X - 8X 1064 / 532 4.5 - 11 36 45 - 50 114 - 142 6-BE-T-1064-532 1450€

Tunable 2X - 11X 800 / 400 4.5 - 11 36 45 - 50 112 - 142 6-BE-T-800-400 1450€

Catalog Items

Beam expander for any wavelength from 266 - 2000 nm spectral range available on request.


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MOTEX - MOTORIZED TUNABLE BEAM EXPANDER Specifications

Features

• Aberration minimized design (special aberration compensation layout)

• Plug & play solution (controller included)• Suitable for ultrafast picosecond and femtosecond lasers • Direct control from microcontrollers and embedded

systems • Optional adjustable mounting interface• Individual calibration capability• Individual presets for magnification • Reduced setup time by automatic magnification adjustment•Manual magnification control

Applications

• Laser beam size control in industrial and scientific applications, laser machining systems

• Automatic control of focusing parameters (Numerical Aperture)

• Hands free operation in remote machinery places and hazardous conditions

Catalog Items

Wavelength, nm Product ID Price

1020 – 1070 MBE-1 2225€

510 – 540 MBE-2 2225 €

340 – 360 MBE-3 2225 €

Lens materialOptical crown glass or UV grade fused silica

Continously variable magnification

2.5x…12x

Wavelength range1020 – 1070 nm510 – 540 nm340 – 360 nm

Entrance beam diameter up to 10 mm

Output beam diameter up to 48 mm

Overall transmission 98.5 %

LIDT >7 J/cm2 for 10 ns pulses @ 1064 nm

Control interfaces USB 2.0; UART (RS232); Step/Dir

Software platform WindowsTM

Weight 1 kg


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• Holography• Information processing • Marking and engraving • I llumination • Particle image velocimetry • Particle size analyzing • Geochronolgy •Pumping of Ti:Sapphire lasers and amplifiers

LASER BEAM SHAPING SYSTEMS

piShaper produces a collimated flat-top beam over a large working distance. With this unique tools it is possible to convert a Gaussian laser beam into a collimated flattop (or top-hat) beam with nearly 100% efficiency.

The main benefit of using piShaper is saving of laser energy what is very important in many laser applications, especially in material processing. The problem is that the Gaussian intensity distribution is not an optimum one in many cases. From this point of view evaluation of the efficiency of using laser energy has a great importance.

BASIC PRINCIPLES OF OPERATION:• piShapers are telescopic or collimator optical systems that

transform Gaussian intensity distribution of source laser beam to a flattop one;

• Achromatic design provides this transformation for a certain wavelength range;

• Galilean design, thus there is no intermediate focusing of a

beam;

Description

• Flow cytometry • Free electron lasers • Mass-spectrometry • Laser annealing • Welding of metals and plastics • Soldering • Laser cleaning

Laser beam shaping systems for micromachining applications The best choice for manipulation of focused beam is Focal-piShaper_xxx. “Flattop”, “donut”, “Inverse Gauss”, “Trident”, “Roof ” and other shapes can be created in the focal region of any diffraction limited lens.


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Product ID TypeInput gaussian beam,

1/e2 levelOutput flattop beam

Wavelength range*, nm

Application based on

piShaper 6_6_series

piShaper_6_6_VIS Telescope 6 mm collimated 6 mm collimated 420-680He-Ne, He-Cd and other lasers

of visual range

piShaper_6_6_TiS Telescope 6 mm collimated 6 mm collimated 660-1040Ti:Sapphire laser and other

near IR lasers

piShaper_6_6_852 Telescope 6 mm collimated 6 mm collimated 800-900Ti:Sapphire laser and other

near IR lasers

piShaper_6_6_ 532/1064 Telescope 6 mm collimated 6 mm collimated 520-550

1020-11001st (1064) and 2nd (532)

harmonics of Nd:YAG laser

piShaper_6_6_410/820 Telescope 6 mm collimated 6 mm collimated400-420 800-840

1st (820) and 2nd (410) harmonics of Ti:Sapphire

piShaper_6_6_1319 Telescope 6 mm collimated 6 mm collimated 1200-1400 near IR laser diode sources

piShaper_6_6_1550 Telescope 6 mm collimated 6 mm collimated 1500-1600 near IR laser diode sources

piShaper_6_6_350 Telescope 6 mm collimated 6 mm collimated 330-3703rd (355 nm) harmonic

of Nd:YAG and similar lasers

piShaper_6_6_350_C Collimator 75 mrad divergent 6 mm collimated 330-3703rd (355 nm) harmonic

of Nd:YAG and similar lasers

piShaper_ 5.6_6_series

piShaper_5.6_6_1064_HP Telescope 5.6 mm collimated 6 mm collimated 1020-1100High power fiber, Nd:YAG and

other near IR lasers

piShaper_ 37_34_series

piShaper_37_34_1064 Collimator 180 mrad divergent 34 mm collimated 1020-1100High power fiber lasers fiber-cou-

pled diode and DPSS lasers

piShaper_ 4.5_4.5_series

piShaper_4.5_4.5_1064C Collimator 180 mrad divergent 4.5 mm collimated 1020-1100Nd:YAG, fiber and other

near IR lasers

piShaper_5_6_series

piShaper_5_6_VIS Telescope 5.8 mm collimated 6 mm collimated 340-5602nd, 3rd harmonics Nd:YAG lasers,

lasers of visual range

piShaper_12_12_series

piShaper_12_12_1064_C Collimator 58 mrad divergent 12 mm collimated 1020-1100Nd:YAG, fiber and other

near IR lasers

piShaper_12_12_TiS Telescope 11.9 - 12.0 mm collimated 12 mm collimated 700-900Ti:Sapphire laser and other

near IR lasers

piShaper_12_12_TiS_C Collimator 60 mrad divergent 12 mm collimated 700-900Ti:Sapphire laser and other

near IR lasers

piShaper_12_12_355 Telescope 12.2 mm collimated 12 mm collimated 330-3803rd (355 nm) harmonic of Nd:YAG

and similar lasers

piShaper_12_12_355C Collimator 60.5 mrad divergent 12 mmcollimated 330-3803rd (355 nm) harmonic of Nd:YAG

and similar lasers

piShaper_12_12_266 Telescope 12.2 mm collimated 12 mm collimated 250-2704th (266 nm) harmonic of Nd:YAG

and similar lasers

piShaper_12_12_266C Collimator 60.5 mrad divergent 12 mm collimated 250-2704th (266 nm) harmonic of Nd:YAG

and similar lasers

Catalog Items


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Product ID TypeInput gaussian beam,

1/e2 levelOutput flattop beam

Wavelength range*, nm

Application based on

F-piShaper 9 series

F-piShaper 9_1064 Telescope 5...8 mm collimated <16 mm collimated 1020 - 1100Nd:YAG, Fiber and other

near IR-lasers

F-piShaper 9_TiS Telescope 5...8 mm collimated <16 mm collimated 750 - 850Ti:Sapphire laser and other

near IR lasers

F-piShaper 9_532 Telescope 5...8 mm collimated <16 mm collimated 520 - 5502nd (532) harmonics of

Nd:YAG and similar lasers

F-piShaper 9_355 Telescope 5...8 mm collimated <16 mm collimated 330 - 3803rd (355) harmonics of

Nd:YAG and similar lasers

Accesories

zBeam_9 Zoom beam-

expander < 16 mm collimated

Magnifica-tion

0.75 - 1.33 400-1200

5KOM5F-15-axis Ad-justment

Miscellaneous

• Custom design Laser beam shaping systems are available in small and mass production quantities

Fill the request form at our website to request laser beam shaping systems

* Optimum wavelength range according to coatings applied


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AUTOCORRELATORS

The Autocorrelator is a nonlinear optical device, which measures temporal pulse shape in real time of single ultrashort light pulse with duration from 50 fs to 40 ps. The method used in the Autocorrelator is based on the noncollinear second harmonic (SH) generation, where the spatial distribution of the SH light contains information on the time behavior of the fundamental light pulse. This technique combines the zero background and the single-shot measurement capability. For immediate observation of pulse duration it is convenient to use the photodiode array.

The Autocorrelator can be used with many of today’s ultrashort pulse lasers. The Autocorrelator can be constructed for temporal shape measurements of the pulses with duration down to 30 fs in the spectral range from 523 nm to 1400 nm and with lower temporal resolution in the spectral range up to 4000 nm.

Description

Related products and accessories• High-speed photodetectors (page 194)

Miscellaneous

Features

• Easy to align and operate• Background - free measurement of a pulse duration from

single-shot• Measurement of the non reproducible ultrashort light pulses• Measurement of pulse duration in a wide spectral range• Pulse chirp measurement from a single-shot• Estimation of the chirp pulse compressor adjustment from

single-shot• Fully compatible with a photodiode array for automatic SH

beam pattern recording• Cheap in comparison with a streak camera

• Custom design autocorrelator are available in small and mass production quantities

Fill the request form at our website to request autocorrelators!


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Femtosecond scanning autocorrelators

Product ID 6-AA-10DDV 6-AA-10DD 6-AA-10DDR 6-AA-10DDM

Wavelength range 450-700 nm 700-1300 nm 1300-2000 nm 450-2000 nm*

Pulse duration range 10-6000 fs

Input repetition rate >8 kHz

Input polarization, linear horizontal (vertical upon request)

Scanning rate 0.1-20 Hz

Sensitivity 100 mW2

Linear distortion <1%

Collinear (interferometric and intensity) autocorrelation

yes

PC donnection USB

Necessary equipment PC with Windows OS or oscilloscope

Fiber input (Optional) FC/PC or FC/APC (other types available upon request)

Signal source and detector Two-photon conductivity in semiconductor

Dimensions132x123x118 mm225x190x45 mm (electronic unit)

132x123x118 mm225x190x45 mm (electronic unit)

132x123x118mm225x190x45 mm (electronic unit)

195x166x130 mm225x190x45 mm(electronic unit)

* - model 6-AA-10DDM may cover either all three ranges (450-2000 nm) or two separate ranges (i.e. 450-1300 or 700-2000) with interchangeable optics

and photodetectors (3 or 2 sets included).

Single-Shot femtosecond autocorrelators

Product ID 6-SSNA-1.06 6-SSNA-0.75-1.1 6-SSNA-0.76-0.86 6-SSNA-0.56-0.62 6-SSNA-0.53

Wavelength Range 1040 - 1080 nm 750 - 1100 nm 760 - 860 nm 560 - 620 nm 520 - 540 nm

Pulse Duration Range 50 – 40 000 fs 50 – 12 000 fs 50 – 5000 fs 50 – 7000 fs 50 – 4000 fs

Input Pulse Energy 50 µJ 80 µJ

Processing USB controller

* - other wavelength and pulse duration ranges available on request


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HIGH POWER LASER SHUTTERS

Laser shutter “Katana” is designed for fast single interruption or multiple exposure of high power laser beam.

Operation of high power laser shutter “Katana” is based on the fast galvanomagnetic scanner to achieve speed of blanking better than parts of milliseconds.

Possible applications: laser cutting, drilling, engraving, laser surgery systems, research and others.

Description


• Beam dumps (page 197)

Miscellaneous

• Custom design high power laser shutter is available in small and mass production quantities

• High power laser shutter is also available upon request

Incident beam diameter ≤10-30 M

Wavelength 266, 355, 532, 1064, 10600 nm

Laser power, max 15 W

Switching frequency range (max) 0-1 kHz

Switching time (closed-opened) < 0.2 ms

Typical switching time (opened-opened) 0.4 ms

Typical switching time after command is sent)

3 ms

Control via RS232 port, TTL signal Yes

Control from external (0-5V) generator

Yes

Shutter dimensions80 x 60 x 50 mm185 x 40 x 60 mm

Electronic box (max) 240 x 112 x 68 mm

Laser Energy Ratings up to 10 W/mm2

Standard specifications Catalog Items

Product ID Operation wavelength, nm Price

6-LS-10.6 10600 4200€6-LS-1064 1064 3290€

6-LS-266 266 3520€

6-LS-355 355 3490€

6-LS-532 532 3320€


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BEAM DUMPS

Air and water-cooled beam dumps are designed to block CW or a pulsed laser beam.

Air cooled beam Dump 10BD01 is designed to block a CW or a pulsed laser beam. It can be used on beams of up to 50 Watts in the wavelength range from 0.1 to 30 µm. The design is such, that, even if the non-reflective coating is damaged by high intensity pulses, there’s no backward reflection.

Water-cooled beam dump 10BDWC01-2. Beam dump 10BDWC01 blocks a CW or a pulsed laser beam. It is mainly intended for beams 2 inch wide. Water absorbs much energy. The wavelength range is from 0.1 to 30 m. Even if the non-reflective coating is damaged by high intensity pulses, the laser beam is not reflected back into your optical scheme. Laser beam dump mounts on an M6 hole on its back.

Description

Miscellaneous

• Custom design beam dumps are available in small and mass production quantities

• Custom beam dumps are also available upon request

Wavelength Range, µm 0.1 – 30

Power stand, W 50

Power stand for water-cooled, kW 1

Weight, kg 0.57 / 1.2 for water-cooled

Product ID Power stand, W Price

6-10BD01 50 169€6-10BDWC01-2 1000 239€


Catalog Items

Fill the request form at our website to request beam dump!


• High power laser shutters (page 196)


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IR VIEWER

Altechna offers low cost, compact battery operated IR viewers. This device allows viewing continuous lasers radiation as well as pulsed lasers radiation with pulse duration from ps to μs without synchronization.

* Standard kit includes: IR viewer, IR filter, battery, handle, case.Optional accessories: facemask for hands free operation, infrared illuminator, neutral density filter, iris diaphragm, adapter to AAA, batteries (for IR1700V3 and IR2000V3 viewers), microscope adapter, video adapter VA-1.

Spectral Sensitivity

Catalog Items

Features

• High performance • Compact (0.28 – 0.42 kg)• Low cost (starting from 800€)• Wide spectral range (from 350 nm to 2000 nm)

Spectral sensitivity, nm Resolution (center), lp/mm Field of view, deg Magnification Objective lens Product ID Price

350 - 1300 60 40 1X F1.4/26 mm without iris 6-IR1300V1 800€

350 - 1300 60 20 2X F2/50 mm with iris 6-IR1300V2 870€



350 - 1700 50 25 1.8X F1.4/26 mm 6-IR1700V3 860€



350 - 2000 50 25 1.8X F1.4/26 mm 6-IR2000V3 1190€


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Spectral sensitivity, nm Resolution (center), lp/mm Field of view, deg Magnification Objective lens Product ID Price





350 - 1700 50 25 1.8X F1.4/26 mm 6-IR1700V3 860€



350 - 2000 50 25 1.8X F1.4/26 mm 6-IR2000V3 1190€

Spectral range, nm Emission light colorThreshold sensitivity,

W/cm2

Operational aperture, mm

Product ID Price

880 - 1070 Green 0.0215

6-IRV55€

35 68€

190 - 1600 + 1470 - 1600 Red 0.0115

6-UVIRV65€

35 86€

900-1350 Green to Red 0.1 35 6-IRVQ 90€

190 - 1600 + 1470 - 1600/ 880 - 1070 Red / Green 0.02 / 0.01 35 6-UVIRV/ IRV-Twin 135€780 - 1600 Green 0.05 20x15 6-IRV card 25€190 - 1000 Blue/ Red 0.02 35 6-UVB 90€

Catalog Items

Miscellaneous

• One of the best selling products in 2012!• Custom design laser beam visualizers are available in small

and mass production quantities• Laser beam visualizers are also available upon request

LASER BEAM VISUALIZERS

A visualizer provides luminescent conversion of the invisible IR and UV light to the red, the dependence of the luminescent emission intensity on the visualized light intensity is nonlinear.Currently we are offering 6 types of visualizers:

UVIRV model of Visualizer is intended for visualization of IR and UV coherent and incoherent radiation both from laser and other type-light sources. Visualizer requires no electrical power supply. It is an ecologically-safe ceramic tablet made of rare-earth element compounds.

IRV model of visualizer is designed for conversion of near IR radiation of pulsed and CW lasers to visible green light.The material of visualizer is special ceramic with anti-stokes luminophores.

UVIRV-IRV Twin model combines two models (1 and 2) in one visualizer for your convenience. One side of the visualizer is for UV-IRV visualization (emitting red color) and the other side is for IRV visualization (emitting green color)

IRV card model of visualizer has similar characteristics as the IRV visualizer above but it is not mounted in a holder. Instead it is integrated in a custom design card.

Description

UVB model of visualizer is designed for UV radiation below 266 nm conversion to blue light. Material of UVB is special ceramic with luminophores.

IRVQ model is designed for near IR pulsed radiation conversion into second harmonic. Material of IRVQ is organic polycrystals.


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SPECTACLES AND GOGGLE TYPE SAFETY GLASSES

WARNING: Don‘t look into the laser beam with your remaining eye, better wear our safety glasses!

Working with lasers is entirely safe as long as you apply adequate protection to your eyesight. Otherwise, laser beam impact can induce severe and often irreversible damage to retina or cornea. Take advantage of our professional anti-laser spectacles and goggles. They are comfortable and absolutely safe (if selected properly).

Selecting appropriate laser eye protection

The choice of the most suitable safety spectacles of goggles must be done in compliance with standard EN 166, EN 207 and EN 208. The use of unsuitable eye-wear is one of the most frequent causes of eye injury. So, please, consider the following as a guide. For a correct judgement of optical hazards, it is important to know some fundamental parameters defined in the standards of eye-protection against laser radiation.

Description

• Laser wavelength. Determine all wavelengths to protect against with one pair of glasses

• Output parameters. For continuous wave lasers check the maximum output power and beam diameter to calculate the power density ( W/m2). For pulsed lasers determine the maximum energy, the beam diameter, and the frequency (if applicable) to calculate the energy density (J/m2) or power density

• Spectral transmittance and optical density. Spectral Transmittance is the ratio between the power (or energy) transmitted by the filter and the incident power. Find recommended minimum power (or energy) density value that the protection filter must comply with in the standard EN 166, EN 207 or EN 208 tables - the closest greater value to your calculation. Optical density relates to transmission by equation: D = -log10 T.

EUROPEAN STANDARD EN 207 - Classification and specifications of filters and eye protection against laser radiation

Optical densityscale number

Spectral transmit-

tance

Conditions of stability to laser radiation180 nm ≤ λ ≤ 315 nm 315 nm ≤ λ ≤ 1400 nm 1400 nm ≤ λ ≤ 10.6 μm

DW/m2

I,RW/m2

MW/m2

DW/m2

I,RW/m2

MW/m2

DW/m2

I,RW/m2

MW/m2

L1 10-1 10-2 3x102 3x1011 102 5x10-2 5x107 104 103 1012

L2 10-2 10-1 3x103 3x1012 103 5x10-1 5x108 105 104 1013

L3 10-3 1 3x104 3x1013 104 5 5x109 106 105 1014

L4 10-4 10 3x105 3x1014 105 50 5x1010 107 106 1015

L5 10-5 102 3x106 3x1015 106 5x102 5x1011 108 107 1016

L6 10-6 103 3x107 3x1016 107 5x103 5x1012 109 108 1017

L7 10-7 104 3x108 3x1017 108 5x104 5x1013 1010 109 1018

L8 10-8 105 3x109 3x1018 109 5x105 5x1014 1011 1010 1019

L9 10-9 106 3x1010 3x1019 1010 5x106 5x1015 1012 1011 1020

L10 10-10 107 3x1011 3x1020 1011 5x107 5x1016 1013 1012 1021

D - continous wave lasers; R - giant pulsed lasers (Q - switching; 10-9 s < t < 10-7 s); I - pulsed lasers (10-4 s < t < 10-1 s); M - giant pulsed lasers (Mode - locking; t < 10-9 s).


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λ, nm ODColour of

filterTransmittance in visible range

Product ID Price

190 - 380 nm 9000 - 11000 nm

5+ 7+

Clear 90% 6-SG-EC3 105€

190 - 398 nm 10600 nm

7+ 5+

Clear 93% 6-SG-EC2 65€

180 - 532 nm 7+ Orange 48% 6-SG-ARG 70€

190 - 534 nm 790 - 850 nm

>960 - 1070 nm 765 - 1090 nm >850 - 960 nm

7+ 7+ 7+ 5+ 6+

Amber 22% 6-SG-DBD 165€

190 - 435 nm 730 - 1085 nm

755 nm 1064 nm

5+ 5+ 7+ 7+

Green 36% 6-SG-CYN 120€

190 - 400 nm 615 - 720 nm 651 - 670 nm 671 - 715 nm 680 - 710 nm 690 - 700 nm

6+ 3+ 4+ 5+ 6+ 7+

Teal 35% 6-SG-RB2 110€

190 - 400 nm 670 - 695 nm

815 - 1050 nm 1050 - 1080 nm

5+ 3+ 3+ 2+

Green 35% 6-SG-DI6 105€

190 - 400 nm 630 - 660 nm 800 - 915 nm 780 - 920 nm

5+ 3+ 3+ 2+

Blue-Grey 19% 6-SG-ML3 110€

190 - 380 nm 950 - 1070 nm 808 - 840 nm

>840 - 950 nm 1064 nm

2700 - 2950 nm

5+ 7+ 4+ 5+ 7+ 5+

Green 59% 6-SG-YRB 195€

Catalog Items

λ, nm ODColour of


Product ID Price

850 - 5200 nm 945 - 2300 nm

2300 - 2500 nm 2800 - 10600 nm 1010 - 1500 nm

3+ 5+ 4+ 5+ 7+

Green 75% 6-SG-FG1 265€

190 - 534 nm 960 - 1064 nm 925 - 1070 nm 850 - 925 nm

7+ 7+ 6+ 5+

Green 59% 6-SG-DBY 150€

190-400 nm 808-840 nm

>840-950 nm >950-1070nm

>1070-1090nm

5+ 4+ 5+ 7+ 5+

Green 35% 6-SG-YG3 120€

180 - 400 nm 720 - 1090 nm 750 - 1064 nm

6+ 5+ 7+

Amber 25% 6-SG-YG2 130€

190 - 400 nm 625 - 647 nm 630 - 644 nm

5+ 5+ 6+

Blue 18% 6-SG-HNE 110€

190 - 400 nm 720 - 810 nm

>810 - 830 nm

6+ 7+ 5+

Pink 33% 6-SG-AXX 120€

190 - 400 nm 532 nm

910 - 1070 nm 850 - 1075 nm 808 - 850 nm

5+ 3+ 6+ 5+ 4+

Orange 33% 6-SG-YGN 150€

190 - 400 nm 785 - 830 nm

830 - 1700 nm

5+ 2+ 3+

Yellow/Green

23% 6-SG-IRD 115€

180 - 400 nm 450 - 470 nm

532 nm

5+ 2+ 3+

Orange 38% 6-SG-ABG 110€


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Miscellaneous

• EN 166, EN 207 and EN 208 certified• One of the best-selling products in 2012• Custom design spectacles are also available • Choose the most suitable design of frames


• Laser diodes (page 203)


• Motorized Watt Pilot attenuator (page 193)

6-SG-33

6-SG-38

6-SG-34

6-SG-51

Styles of safety goggles:

λ, nm ODColour of


Product ID Price

180 - 534 nm 770 - 850 nm 720 - 770 nm

850 - 1080 nm 750 - 760 nm

980 - 1064 nm

7+ 4+ 5+ 5+ 5+ 7+ 7+

Amber 26% 6-SG-TRI 170€

180 - 534 nm 720 - 730 nm

>730 - 740 nm >740 - 1070 nm

7+ 5+ 6+ 7+

Amber 11% 6-SG-YAD 200€

Catalog Items


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Features

• Configurable with different customized wavelengths up to 130W output power

• Individually addressable wavelengths through a single fiber• Monitor Photodiodes• Active or Passive cooling options

LASER DIODES AND MODULES

ALTECHNA offers full service in selecting the right laser diodes and necessary accessories for clients’ applications. Ahead with engineers of High power laser diode driver ALTECHNA gives opportunity to have all setup from one hands. High power single-emitter laser diode modules in wavelengths from 790 nm to 1064 nm are available together with various fiber jacket and connector options. Mount kit, test software and copper air-cooled heat sink are available separately. Several different wavelengths coming out of the same fiber, including a red or green guide light is available as well.

Fiber coupled single emitter modulesSingle fiber output up to 9 W in a package smaller than a dime is available in fiber diameters of 50 µm and 105 µm.

Laser diode up to 50 W of output powerAir-cooled or water-cooled, single or bundled fiber output up to 50 W from 200 µm / 0.22 NA fiber in a 140 mm x 100 mm package.

Laser diode up to 70 W of output powerAir-cooled or water-cooled, single or bundled fiber output up to 70 W from 300 µm or 400 µm / 0.22 NA fiber in a 196 mm x 100 mm package.

Laser diode up to 130 W of output powerAir-cooled or water-cooled, single or bundled fiber output up to 130 W from 400 µm / 0.22 NA fiber in a package smaller than a notebook computer.

Description

Contact ALTECHNA for more information about laser diodes and modules, available models and pricing [email protected]


• High power laser diode DRIVER for DPSS lasers (page 179)


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OPTICAL CHOPPERDescription

Optical chopper is a device used for a mechanical modulation of light beam. Slotted mechanical disc rotates thanks to a highly stabilized motor. Through the disc a light beam is passing and being modulated. The rotations are controlled with a usage of a dedicated controller connected with chopper head through a cable.The modulation speed can be adjusted using local keyboard or USB/Serial port. The device generates very low noise and has low modulation head dimensions. It contains also the synchronisation output, which enables cooperation with lock-in-amplifiers.

Computer Software

A dedicated software with a friendly GUI is added. It allows to perform all operations on the chopper. Software works in Microsoft Windows and Linux environment. It is designed to automatically find all connected and switched on devices.


The standard set contains

• Chopping head• Controller unit• Software for PC• Interconnecting cable (chopping head – controller unit)• Mains leads (220V ,50Hz)• Chopping disc (2, 4, 8, 16)• Range of frequencies: Disk with 2 slots: 0 Hz-150 Hz Disk with 4 slots: 0 Hz-300 Hz Disk with 8 slots: 0 Hz-600 Hz Disk with 16 slots: 0 Hz-1000 Hz• Other slots disc on request

Product ID Disks Range of frequencies Price

OM-USB-2.1 4 0 Hz-1000 Hz 760€

Modulation speed 0.1 - 3000 Hz

Speed controldigital (embedded keyboardand LCD or RS232/USB)

Stability ± 0.1 %

Aperture 18 mm

Interfaces RS 232, USB

Synchronization output BNC, 5V TTL

Supply24V DC, 90..250VAC, attached

mains adaptor

Dimensions:

Diamter of the disc (outermost) 120 mm

Thickness of the head with a disc 27 mm

Width of the slot (for discs with 2, 4, 8 slots)

15 mm

Width of the slot (for discs with 16 slots) 9.8 mm

OptOmechanics

OpticaL taBLes 206

Base mOUnts anD accessORies 207

•post mountings 207

•adapters 208

•post collars, clamps and base plates 208

OpticaL mOUnts anD hOLDeRs 211

•Optical mounts 211

•Optics holders 213

OpticaL pOsitiOneRs 215

•stainless steel kinematic mounts 215

•Repositioning mounts 217

•polarizer holders 218

•2 axis tilt mounts 220

•precision optical mounts of side control 222

•2/3 axis tilt / translation mounts 223

•mirror mounts/ tilt platforms of side drive 226

•miniature precision mirror mounts 228

•special positioners 229

•Budget kinematic optical mounts 231

Base pOsitiOneRs 232

tRansLatiOn & ROtatiOn staGes 234

•Rotation stages 234

•narrow translation stages 236

•Low profile translation stages 237

•micro translation stages 239

•Vertical positioners 239

•Dovetail linear translation stages 240

mOtORiZeD pOsitiOneRs anD cOntROL-LeRs

241

•translation stages 241

•Rotation stages 244

•Vertical translation stages 248

mOtORiZeD attenUatORs 254


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OpticaL taBLesDescription

altechna offers a wide range of optomechanical products in-cluding optical tables, brackets&rails, base mounts&accessories, optical mounts, optical positioners, base positioners, transla-tions & rotation stages, motorized positioners & controllers, fine adjustment screws and opto-mechanics&sets. these products are used for various scientific and industrial applications requir-ing features such as: precision, stability, corrosion resistance, vi-bration isolation and damping and many more.

here in our catalogue you can find only small part of our opto-mechanical products. all of our standard opto-mechanical prod-ucts are described in detail in our website www.altechna.com

Honeycomb table tops provide the base on which precision optical and laser work is performed. the table tops have a hon-eycomb core inside. the table tops meet high requirements for rigidity, flatness, vibration isolation and damping.

non-magnetic optical tables

pneumatic vibration isolation system

pneumatic vibration isolation workstation

table connectorBreadboard mounted on a table by silent rods

Honeycomb breadboards provide a particularly effective way to expand the useful area of an optical table.

We offer optimal vibration isolation systems for the optical table of your choice.

Pneumatic vibration isolation systems ensure low resonant fre-quency almost independent of load. they have automatic level-ing valves and an autonomous air supply reservoir. the pressure in isolators varies with the load.

Pneumatic vibration isolation workstation consists of a honey-comb Breadboard, and a guarding armrest. workstation has an automatic leveling valve and an autonomous air supply reser-voir.as you lean on the armrest, it guards the honeycomb table from impacts of your body. this allows you to work at the table like at a conventional table, using microscope and other equip-ment.

Table connectors render quick and reliable way to link table tops together.


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Base mOUnts & accessORies

post mountings

posts and post holders provide a simple means for mounting op-tical components. they may be stud mounted to a wide variety of component holders.

stainless steel Mounting posts 3MP and 3SMP have m4 and m6 holes on the ends. components can be mounted using screws or 3AH adapters for different threads. each post can be attached directly to a base surface using adapters 3ah. mounting posts could be used together with post holders 3ph.

special mounting post 3SMP and 3MP-05-3 riser post are de-signed for small units.

3MP4-20 and 3MP4-47 posts have an external m4 end.

special mounting post 3SMP4-47 is designed for little optical mounts, which have no space for the Ø12mm rod.

3mp, 3smp - mounting posts

post holder 3ph, phB

3Utc clamp and post holder 3phB

aluminium post holders 3PH have a precise mounting opening for mounting posts 12 mm in diameter. it provides two lines of contact, thus the position of a precision mounting post be-comes definite. a mounting post is locked in position by a screw (included).

product iD Length (L), mm

Diameter (D), mm

Diameter (d), mm

price

3mp-150 150 12 - 7.30€

3mp-100 100 12 - 6.30€

3mp-75 75 12 - 5.80€

3mp-50 50 12 - 5.50€

3mp-25 25 12 - 5.00€

3mp4-20 20 12 - 6.00€

3smp4-47 47 12 - 10.00€

3ph(B)-100 100 24 12 17.00€

3ph(B)-75 75 24 12 16.00€

3ph(B)-50 50 24 12 14.00€

3ph(B)-33 33 24 12 13.00€

the post hoders 3ph can be mounted to other components us-ing screws, or to breadboards and tables directly using adapters 3AH.

Post holders 3PHB offers more usage convenience and flex-ibility. Design is modified by introducing a slot, which allows clamping post holders to mounting surface using clamps like 3UTC, with no additional parts required.


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Adapters 3AH connect components when precise orientation in plane is not required some adapter have diferent threads on ends.components can be connected with m3, m4, m6, m8 threaded holes. these 3AH adapters are used with mounting posts like 3ph or 3mp.

product iD a D

3ah4-4 m4 2

3ah6-6 m6 3

3ah8-32 8-32 5/6

3ah1/4-20 ¼-20 1/8

product iD a B c D

3ah4-3 m4 m3 2 1.5

3ah6-4 m6 m4 3 2

3ah8-4 m8 m4 4 2

3ah8-32-1/4-20 8-32 ¼-20 5/64 1/8

* c and D denote hex key sizes

thread adapters 3ah

post collar, clamps and base plates

Post collars 3PC8 are offered separately to hold the posts at a preset height. placing an aluminium post collar 3pc onto the posts at specific height allows the post to be rotated without changing height. it fits Ø12 mm posts.

product iDLength (L), mm

Diameter (ØD), mm

aperture (Ød), mm

price

3pc8 15 20 12 8€

post collar

Universal Fork Clamp 3UTC is used for mounting 2sR32 rods or 3mp25 pedestals to tables, you may use 3ah adapters and 3Utc clamp.

Universal fork clamp 3Utc


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Adjustable angle post clamp 3APC allows mounting posts 3mp of Ø12 mm and silent rods of Ø32 mm to be mounted to one another at any angle and then securely locked in position with independent thumbscrews.

adjustable angle post clamp 3apc

adjustable angle post clamp 3apc-12-3 is used

Rotary Clamp 3EXC45 is used to fasten components at random positions where they cannot be fastened directly to the optical table.screw a post or post holder onto theclamp’s knob. then locate the componentat the required position. While the knobis firmly attached to the component, it allowsthe plate to rotate freely. position theplate’s slot over a tapped hole and screw it-down to clutch the knob. the componentwill remain stable.

Rotary clamp 3eXc45

Using Table Clamps 3TC5 you can position any base and most base mounted components at any angle on the table and have not to be limited by mounting hole pattern of the optical table.

product iD materialDimensions,

mmprice

3Utc stainless steel 25 x 57 15€

3apc-12-12 black anodized

aluminium47 x 51 20€

3apc-12-32black anodized

aluminium63 x 85 39€

3eXc45steel , chemical

black finish26 x 57 8€

3tc5steel , chemical

black finish50 x 16 10€

table clamp 3tc5


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Base plates 3BP4 are designed to position posts and holders. the base is fastened by mounting slots, which allow to slide the base to positions independent of the pattern holes.

Low-profile magnetic base 3MB6 has a high holding force that does not degrade with time, a low profile, generous mounting provisions, a non-magnetic mounting surface of the magnetic base, a holding force which you may vary continuously by the easy to reach inset adjustment screw. an exclusive stable mag-netic circuit ensures that the magnetic elements move linearly.

product iD materialDimensions,

mmprice

3Bp4-01 steel of black finish,

or black anodized

aluminium

50 x 25 x 9 4.80€

3Bp4-02 76 x 25 x 9 5.20€

3RBp-39 Ø 39 7.00€

3RBp-49 Ø 49 7.00€

3cmB4-19* - Ø 19 10.00€

3cmB6-19* - Ø 19 10.00€

3cmB4-27** - Ø 27 16.00€

3cmB6-27** - Ø 27 16.00€

3mB6*** - 125 x 125 x 44 332€

*- highest holding force up to 5 kg**- highest holding force up to 10 kg***-highest holding force up to 140 kg

Round base plates 3RBP are used for mounting posts and posts holders to position them at random. the post stays stable with-out fastening. if required, the plate can be fastened using table clamps.

Magnetic bases 3CMB are very useful for small components that may be quickly positioned on ferromagnetic optical tables, breadboards or translation stages.

Base plates 3Bp4

Low-profile magnetic base 3mB6

Round base plates 3RBp

magnetic bases 3cmB


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OpticaL mOUnts anD hOLDeRs

altechna offers various optical mounts and optics holders such as self-centering optics mounts for lenses, simple optical component mounts for various round, standard dimensions optics elements, adjustable radius optics mount for round objects of virtually any thick-ness and length and big optical mounts for large and heavy elements.

optical mounts

Self-centering lens / optics mount 4LM13, 4SCML reliably cen-ters and securely holds round optics and cylindrical objects. this device is particularly valuable when lenses of different di-ameters are being used interchangeably, as repeated centering at constant height is necessary. Optical elements are fixed and centered at the same time by adjusting driving screw at the top of the device. heavy optics mounting is secured by wedged rods.

Self-centering optics mount 4SCML accommodates optics with large aperture – up to 305 mm (4scmL-8) in diameter. Optics can be round or cylindrical shape.

Features:

• automatically centers and holds optics from 6 to 40 mm • easy insertion and removal of optics

self-centering lens/optics mount 4Lm13-40

Features:

• 40 mm, 50.8mm, 101.6 mm optics mounts (adjustable range)• 3 mounting holes for fixing to flat object• easy insertion and removal of optics• can be motorized

product iDOptics diameter

range, mmprice

4Lm13-40 Up to 40 75€

4scmL-2 Up to 50.8 99€

4scmL-4 Up to 101.6 140€

4scmL-8 25.4 - 203.2 365€

4scmL-12 76 - 305 2155€

self-centering Lens/Optics mounts 4scmL-12


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Universal adjustable lens / optics mounts 4LM149-10 and 4LM149-05 are used to accommodate any round objects of any thickness like lenses, mirrors and lasers. three support shafts of holder are assembled with non-rotating V-groove aluminium universal interchangeable tips for lenses mirrors, etc. each indi-vidual adjustable shaft of holder incorporates threaded thumb-screw, sliding sleeve and fixation tool for rough positioning and diameter setting Optical component mount 4Ocm can be used to hold round thin optical elements of standard sizes. mounts vary in dimensions so as to support diameters from 10 to 75mm.

Optical Component Mount 4OCM can be used to hold round thin optical elements of standard sizes. mounts vary in dimen-sions so as to support diameters from 10 to 75mm. mounts ma-terial: black aluminium.

product iD

Optics diam-eter, mm

clear aper-ture, mm

hous-ing di-ameter,

mm

D,mm

e,mm

F,mm

price

4Ocm-10 12.7 8 26 12 10 13.5 15€

4Ocm-20 20 17 33 12 10 18.8 18€

4Ocm-25 25.4 23 38 12 10 21.3 17€

4Ocm-40 40 37 53 18 16 28.8 22€

4Ocm-50 50.8 48 65 18 16 34.8 24€

4Ocm-75 75 72 89 18 16 46.5 44€

product iD a, mm B, mm h, mm Optics diameter

range, mm

price

4Lm149-05 134-164 124-141 49.1 10-66 99€

4Lm149-10 164-210 158-185 65.7 38-103 152€

Features:

• hold cylindrical objects of various diameters• Quick coarse positioning and diameter setting possibility• convenient holding of tips not used at the moment• made of black anodized aluminum• three mounting possibilities• Quick coarse positioning and diameter setting possibility

Universal adjustable lens/ optics mount 4Lm149-10

Optical component mount 4Ocm-25


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Multiple filter holder 4FH56 allows fixation of up to 6 filters. the thickness of the optical filter or plate to be held is from 2 mm to 6 mm. the holder is made of black finished steel. separators are made of plastic. m6 tapped mounting holes provide L and V oriented filter positioning.

multiple filter holder 4Fh56

optics holders

Optics holders consists of multiple filter holders which allows fixation of up to 6 filters, push holders for optics of any shape or configura-tion: round and rectangular, with negligible loss of clear aperture, even at large angles of incidence, plate clamps for thin light-weight plates and universal plate holders for long and thick components.

Push holder 4H29 holds optics of any shape or configuration: round and rectangular, with negligible loss of clear aperture, even at large angles of incidence. the top support is clamped in position pushing the special place and tightening the knurled screw. this provides gentle but firm fixation.

Features:

• special method of fixation• holds optics of 12.5 to 42 mm diameter• holds thin lenses or long-barrel lens assemblies• holdsthin lenses or long-barrel lens assemblies

push holder 4h29

Features:

• special method of fixation• holds optics of12.5 mm (0.5”)to 89 mm (3.5”) diameter• clamping screw with V-shapedswivel head• material: black anodizedaluminium

product iDOptics diameter

range, mmprice

4Fh56 - 19€

4h29 13 - 42 44€

4h89 12.5 – 89 89€

adjustable height V-mount 4h89

Adjustable height V-mount 4H89 allows special method of fixa-tion up to 89 mm optics diameter.


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Multiple filter holder 4OFH-10 provides convenient means of working with large number of optical, filters, especially when filters are changed frequently. this holder can mount up to 10 filters.

product iDOptics

diameter, mmOptics

thickness, mmprice

4OFh-10 50.8 (square) 3 92€

4ph132 - Up to 12 53€

4VFh-5-1 25.4 4.5 190€

4VFh-5-2 50.8 4 250€

Variable Filter Holder 4VFH provides a possibility flipping filters in and out of the optical path. Filter replacement is fast and easy. two models are available - for 25.4 (1”) mm and for 50.8 mm (2”) optical filters. maximim filter thickness for 2” models is 4 mm, and 4.5 mm for 2” model. standard models have five slots for filter mounting. all contact surfaces are covered with plastic to prevent scratches.

standard specifications

Filter slots 5

Optics diameter

4VFh-5-1 25.4 mm

4VFh-5-2 50.8 mm

maximum optics thickness

4VFh-5-1 4.5 mm

4VFh-5-2 4 mm

Universal plate holder 4PH132 holds long and thick compo-nents, and can fix elements from 0 to 12 mm in width. the base of the plate holder has an m6 mounting hole.

Features:

• Designed for 2” square Filters• Filter thickness 3mm• can mount 10 Filters• material: black anodizedaluminium

multiple filters holder 4OFh-10

4VFh variable filter holder

Universal plate holder 4ph132

4VFh-5-1 4VFh-5-2


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We offer a broad selection of optical positioners which suit the optical components listed earlier in this catalog as well as many others. Flipping mounts to place optics in and out of the optical scheme. Flip the platform out and back again, and it sits on the driving screws in a repeated position. 2/3 axis tilt/translation mounts suitable for precise alignment of various optical elements to desired angular and linear orientation.

stainless steel kinematic mounts

Vertical drive optical mount is manufactured in two modifica-tions: 5VDOm-1 with flat L-form spring. 5KVDOm-1 with spiral springs.

Ultra-stable kinematic mirror mounts 5VDOM-1 are designed to minimize mount-induced wavefront distortions. in conven-tional mounts, the mirror is tightened by a side screw. Radial forces acting on the mirror induces parasitic wavefront distor-tion, such as astigmatism. 5VDOm-1 mirror mounts use secure 3-points mirror suspension in between frontal flat spring and the back plate. Uniformly distributed axial forces eliminate wavefront distortion.

Due thermal processes on optic holding part, all metal inner tensions were removed and part makes none micro movements.

these mounts are ideal for industrial applications in different optical devices (laser cavities, optical sub-assemblies, limited space applications) because of their long-term stability.

Features:

• 25.4 mm optic diameter• stainless steel• annealed front panel• compact/robust design• super stable with flat spring• motorized version available

Kinematic vertical drive optical mount 5KVDOm

L-shaped spring 5VDOm-1 (left) and spiral spring 5KVDOm-1

OpticaL pOsitiOneRs


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Kinematic vertical drive optical mount 5KVDOM-05 is de-signed to minimize mount-induced wavefront distortions. in conventional mounts, the mirror is tightened by a side screw. Radial forces acting on the mirror induces parasitic wavefront distortion, such as astigmatism. Uniformly distributed axial forc-es eliminate wavefront distortion.

Features:

• For Ø12.7 mm (0.5 inch) optics• stainless steel• compact/robust design• Lockable adjustment screws

product iDOptics diame-ter, mm

Details price

5VDOm-1 25.4 128€

5KVDOm-1 25.4 128€

5KVDOm-2 50.8with supporting

adapter for 12.7mm thickness optics

292€

5KVDOm-2-05 50.8for 8mm thickness

optics292€

5KVDOm-3 76.2with supporting

adapter for 12.7mm thickness optics

350€

5KVDOm-3-05 76.2for 8mm thickness

optics350€

5KVDOm-05 12.7 Optical mount 115€

5KV-DOm-05.10

12.7 Frontal flat spring 10€

5KVDOm-05 Kinematic vertical drive optical mount

5KVDOm-05 5KVDOm-05.10


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Flipping mount 5F21-1 is used to place optics in and out of the optical scheme. Fliping the platform out and back again it sits on the driving screws in a repeated position. precise align-ment of various optical elements to desired angles is done by 2 driving screws. the platform can be fliped either vertically or horizontally.


Fine screw thread m6x0.25

mounting hole 1”

clear aperture 24 mm

maximum optics thickness 7 mm

Repeatability 30 µrad

adjustment range 8°

sensitivity 3arcsec

repositioning mounts

Features:

• Flip optics in and out of the experiment• Kinematic design• precise and handy angular adjustment in two orthogonal

planes• stable vertical mounting• made of black anodized aluminium

Flipping mirror/ beamsplitter mount 5F21-1

Miniature flipping mirror/ beamsplitter mounts 5F23-05 is used to place optics in and out of the optical scheme. this hold-er designed for Ø12.7 and Ø25.4 mm (0.5” and 1”) optics.

miniature flipping mirror/ beamsplitter mounts 5F23-05

product iD accepts optics, mm Fixing price

5F21-1 Ø25.4 135€

5F21-1-sh Ø25.4 9sh127 hex hole

127€

5F21m-1-sh* Ø25.4 127€

5F23-05-sh Ø12.7 99€

5F23-1-sh Ø25.4 104€

5F21m-1* Ø25.49s127

with knobs

135€

5F23m-05-sh* Ø12.7 99€

5F23m-1-sh* Ø25.4 104€

* mirror version

Features:

• Flip optics in and out of the optical scheme• clear edge design suits schemes where beam passes close to

optics’ edge• Kinematic design• high stability

standard specifications:


tilt/tip range 9°

sensitivity 8 arcsec

Repeatability 20 µrad


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adjustable polarizer holder 5aph59t-1

5aph69t-1 (back view) 5aph79t-1 (back view) - the base has aperture for second optics (not

adjustable)

Features:

• Both tilt and tip are controlled from aside the optical path• ideal for dense optical schemes• Fine adjustment screws with 0.25 mm pitch• Roller bearings• Lockable• continuous 360° rotation• horizontal and Vertical mounting

product iD accepts optics, mm price

5aph59t-1 25.4 155€

5aph69t-1 25.4 165€

5aph79t-1 25.4 169€

polarizer holders polarizer holder ’s main function is to rotate polarization optics about the optical axis. adjustable polarizer holders complement our range of polarizers with an integrated adjustment of tilt and tip about two orthogonal axes.

Adjustable polarizer holders 5APH59T-1 complement our range of polarizers with an integrated adjustment of tilt and tip about two orthogonal axes.the holder accepts optics 25.4 mm in diameter. Optics is stopped by a rest-flange inside the central aperture of the platform, and is secured by a threaded retaining ring.

Kinematic adjustable polarizer holder of side drive 5aph69t-1 is similar to 5aph59t-1 adjustable polarizer holder the only differ-ence is that 5aph69t-1 has kinematic design and 5aph59t-1 has L-shaped flat spring. 5aph79t-1 kinematic double optical mount of side drive with adjustable polarizer holder accepts two pieces of optics: on the platform (adjustable), and on the base (not ad-justable). the fixing screw for optics on the base has a plastic tip. a retaining ring m27x1 to fix the optics is included. a tightening key 3K-25 for the retaining ring is available on request.


Fine screw thread: m6x0.25

tilt/tip range ±2.5°(5aph59t-1)

±2°(5aph69t-1

5aph7)9t-1


Rotation range 360°

scale gradation 2°

Optics accepted

Diameter ≤25.4mm

thickness ≤10.5mm



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polarizer holder 5ph51

polarizer holder 5phh50-1

Base of 5PHH50 polarizer holder has beveled sides for fingers to rotate the platformby its knurled edge. You may transform a polarizer holder into a rotation stage.

Polarizer holder 5PH51 is an original mount with revolving conical angular scale on the face of the holder. this enables the user to set the current position on the scale to any chosen angle independently of the position of the holder. the optical element is secured inside central aperture of the platform of the holder by the threaded retaining ring. the zero on the revolving scale is aligned to the desired axis of transmission.

Features:

• Revolving scale resets the angular position• conical scale easily read from a wide angle• continuous 360° rotation• Lockable• Direct mounting of 1” (25.4mm) optics; 2” model available• accepts optics 19 mm thick

product iDOuter

diameter, mm

Optics diameter,

mm

Width, mm

price

5ph51-1 50 25.4 24 82€

5ph51-2 81 50.8 27 139€


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Polarizer Holders 5PH50 are ideal for positioning rotation sensi-tive optics such as polarizers or waveplates. holders are offered for optics 1”, 2” and 3” in diameter. Optics is placed inside central aperture, where it is securely held in place by a threaded retain-ing ring. the position is indicated on two 360° angular scales, with gradation of 2°.

Features:

• for Ø25.4 mm (1 inch) optics• Reset-flange inside the central aperture stops the optic• nylon-tipped fixing screw secures the optic

Features:

• for Ø25.4 mm (1 inch) optics• hard rests make 2 contact points for optimum stability• On one side the edge of the optics stays clear, helpful in

schemes where beams are situated very close to one another

Features:

• 2 engraved scales located on face and outer surfaces• Direct mounting of optics 1”, 2” or 3” in diameter• compact design with roller bearings• horizontal and Vertical mounting• continuous 360° rotation• Lockable

polarizer holder 5ph50

mirror optical mount 5Bm141

Beamsplitter/ mirror mount5Bm131

2 axis tilt mounts are ideally suitable for precise aligning of vari-ous optical elements to desired angular orientation. these mir-ror mounts are designed for 25.4 mm optics.

2 axis tilt mounts

product iD accepts optics price

5aph59t-1 25.4 mm 155€

5aph79t-1 25.4 mm 169€

5ph50-1 25.4 mm 69€

5ph50-1-h* 25.4 mm 69€

5ph50-2 50.8 mm 138€

5ph50-2-h* 50.8 mm 138€

5ph50-3 76.2 mm 210€

5phh50-1 25.4 mm 78€

* Fixing - hex


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product iD Fine screws price

5Bm131e-1-2 2 44€

5Bm131e-1-3 3 53€

5Bm131em-1-2* 2 44€

5Bm131em-1-3* 3 53€

5Bm141e-1-2 2 50€

5Bm141e-1-3 3 59€

5Bm141em-1-2* 2 50€

5Bm141em-1-3* 3 59€

* Fixing - hex

The large aperture optical mount 5LAM124 on its platform has Ø31.8 mm aperture and six m4 mounting holes. it is designed for precise orthogonal adjustment of mirrors. the Large aperture Optical mount 5Lam124-2 on its platform has Ø50 mm aperture and six m4 mounting holes. it is designed for precise kinematics orthogonal adjustment of mirrors.

The objective mount 5OBM119 has W0.8-36 aperture and is used for precise adjustments of standard microscope objective lenses and ensures low-cost positioning of a focus point. also it can be used in the fiber optics.

Features:

• precise and handy two orthogonal angular adjustments• stabile vertical mounting• Various modifications with sensitivity from 10arcsec to 3arcsec

product iD aperture, mm price

5Lam124 31.8 45€

5Lam124-2 51 99€

5Lam124-9s127 31.8 59€

5OBm119 W0.8-36 55€

Features:

• precise and handy two orthogonal angular adjustments• stabile vertical mounting• Various modifications with sensitivity from 10arcsec to 3arcsec

Objective mount 5OBm119

large aperture optical mount 5Lam124


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precision optical mounts of side control

precision kinematic optical mounts are ideally suitable for precise aligning of various optical elements to desired angular orientation. the tilting element is always true-kinematic-registered. the drive screw pushes the alignment mechanism via hardened steel balls. these mounts provide angular range 9° in both orthogonal axes. the precision kinematic optical mounts are produced of aluminium and can be anodized in the color according to your request. Without special note from you will be provided with the black anodized precision kinematic optical mounts.

The objective mounts of side control 5OBM119T has W0.8-36 aperture and is used for precise adjustments of standard micro-scope objective lenses and ensures low-cost positioning of a focus point. also it can be used in the fiber optics.

Objective mounts of side control 5OBm119t

classical objective mounts 5OBm119

The beamsplitters / optics mount 5BM121T is designed to ad-just beamsplitters measuring Ø25 mm.


travel range ± 2°

Fine adjustemnt screws m6x0.25 mm


Features:

• Original L-shaped flat spring• ideal for high density optical schemes• adjustment of both angles is controlled from a single side

product iD price

5Bm121t 63€

5OBm119t 89€

beamsplitters/ optics mount 5Bm121t


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2/3 axis tilt / translation mounts

highly stable precision L-shaped optical mounts are designed on the basis of two angular adjustment mount and are produced of steel with black chemical finishing. these mounts provide pre-loading against the tips of two precise adjustment screws for elimination of backlash and also ensure the absence of the roll coordinate.

Two angular fine adjustment mounts 5OM are used for holding and adjustment about two angular coordinates of orthogonal or round optic. a clamping bar is used to fix optical elements, ensuring gentle but firm clutch.


Fine screw mounting thread m10x1

travel range 9°


Large aperture mount 5BM57 - special holders with two teflon dowel pads and teflon fixing screw.the mount is ideal for pre-cision adjustment of 1” (25,4 mm), 2” (50.8 mm), 3” (76.2 mm), 4” (101.6 mm) or 6” (152.4) mirrors or beamsplitters. the mount comes with 9s65m screw as standard.

Features:

• special flat spring for improved stability versatility and durabil-ity

• left or right hand mountable• Vertical and horizontal mounting

model h, mm hmax, mm price

5Om37-20 0-28 89 80€

5Om37-50 22-52 122 83€

two angular fine adjustment mounts 5Om37-20

Features:


• suitable for 1”, 2”, 3”, 4”, 6” optics• 6° range, sensitivity 5µm

product iDOptics diam-

eter, mm

Resolution per 5° turn

angular, µradprice

5Bm57-1 25.4 160 89€

5Bm57-2 50.8 160 114€

5Bm57-3 72.6 111 147€

5Bm57-4 101.6 87 177€

5Bm57-6 152.4 73 266€

Large aperture mount 5Bm57


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Kinematic mirror/beamsplitter mounts 5MBM24 are used for precise angular and linear alignment of optical elements.

there are two models: one with round (5mBm24-1, 5mBm24-2, 5mBm24-3) and one with square (5mBm24-1sQ, 5mBm24-2sQ, 5mBm24-3sQ) shaped mounting opening.


maximum optics thickness

5mBm24-1 5.5 mm

5mBm24-2 6 mm

5mBm24-3 14 mm


tilt range 9°

travel range 4 mm

sensitivity 3 arcsec or 1 µm

Kinematic mirror / beamsplitter mounts 5MBM21-1 are de-signed for precise alignmentof various optical elements to de-siredangular and linear orientation. modelswith 2 or 3 screws are available.

product iDOptics diam-

eter, mmscrews/hex square price

5mBm21-1-2* 25.4 2 screws - 65€

5mBm21-1-2sh* 25.4 2 hex - 59€

5mBm21-1-3* 25.4 3 screws - 75€

5mBm21-1-3sh* 25.4 3hex - 72€

5mBm24-1-2 25.4 2 screws - 67€

5mBm24-1-2-sQ 25.4 2 screws yes 81€

5mBm24-1-2sh 25.4 2 hex - 65€

5mBm24-1-2sh-sQ

25.4 2 hex yes 79€

5mBm24-1-3 25.4 3 screws - 75€

5mBm24-1-3sh 25.4 3 hex - 72€

5mBm24-2-2 50.8 2 screws - 99€

5mBm24-3-3 76.2 2 screws - 166€

5mBm24m-s1-s2-s3 **

25.4/50.8/76.2 2/3 screws,

hexno/yes call us

* available 50.8 mm version or motorized version** select1 – optics diameter, select2 – fixing and screw/hex

amount (sh- fixing with hex), select3 – optics shape (sQ – for square optics)

Kinematic mirror/ beamsplitter mount 5mBm24-1-3

Kinematic mirror/ beamsplitter mount5mBm24-2-2sQ

Kinematic mirror / beamsplitter mount5mBm21-1

Features:

• precise and easy adjustment, angular in two orthogonal planes, and linear

• stable vertical mounting• made of black anodized aluminium• round and square shaped mounting opening


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Miniature kinematic mirror/beamsplitter mount 5MBM23-05 designed for 12.7mm diameter optics.



tilt/tip range 14°


Features:

• Kinematic• clear edge design• hex key drive• Black anodized aluminium• “mirror” version available

miniature kinematic mirror/beamsplitter mount 5mBm23-05-3sh

Prism mount 5PM57 mounts a platform and allows to hold wid-er optics. positioning features are the same.


Fine screw mounting thread m10x1

travel range 9°


prism/optics mount 5pm57

Features:

• Kinematics, orthogonal angular adjustments• Vertical and horizontal mounting• Left or right hand mountable

Universal prism/ optics mount 5pmF57with bar clamp 4Bc32

product iDaccepts optics,

mmclear

aperture, mmprice

5mBm23-05-3sh Ø12.7 Ø10.2 60€

5mBm23m-05-3sh * Ø12.7 Ø10.2 60€

* mirror version

product iD Options price

5pm57 99€

5pm57 with bar clamp 4Vc41

prism mount call us

5pm57with spring clamp 4sc-52m4

Universal prism / Optics mount

call us

5pm57bar clamp 4Bc32Universal prism /

Optics mountcall us


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Optical filters mount 5FM57 provides fixation and adjustment about two angular coordinates of up to 6 filters. the thickness of optics plate to be held is from 2mm to 6mm. highly stable precision L-shaped Optical mounts are designed on the basis of two angular adjustment mounts, and are produced of steel with black chemical finishing.

Features:


• Kinematics, orthogonal angular adjustments• Vertical and horizontal mounting• Left or right hand mountable

product iD price

5Fm57 60€

Optical filters mount 5Fm57

mirror mounts/tilt platforms of side drive

Small optical mount of side drive 5Om10t is designed to hold optics in schemes of high density. adapters are available for round and rectangular lenses, mirrors and beamsplitters or po-larizing cubes.



tilt range 6°

Rotation range 6°


miniature optical mount of side drive 5Om10t

Mirror mount of side regulation 5OM122T enables to greatly increase the thickness of optical elements as it has a convenient access to the regulation handles.

mirror mounts/ tilt platforms of side drive 5Om122t


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Adjustable beamsplitter mount of side drive 5BM59T-1 ac-cepts optics 25.4 mm in diameter. Optics is stopped by a rest-flange inside the central aperture of the platform, and is secured by a steel hex fixing screw. the fixing screw has a hard plastic tip to prevent damage to the optics. to allow an unimpeded access for your fingers there are two pick-hollows. 3 mounting holes allow different mounting orientations.

specifications


tilt/tip range ±2°


Optics accepted

Diameter Ø25.4 mm (1”)


Features:

• Both tilt and tip are controlled from aside the optical path• ideal for dense optical schemes• Original stabilized L-shaped flat spring• accepts optics 25.4 mm (1”)in diameter• tilt/tip travel range ±2°• two pick-hollows allow keeping grip on optics while reinsert-

ing• horizontal and Vertical mounting

product iD price

5Bm59t-1 85€

5Bm69t-1 87€

5Bm79t-1 90€

Mirror mount of side regulation 5OM122TE. this variant has no clear aperture. this makes it an ideal tilt platform.

product iD price

5Bm121t 63€

5Bm69t-1 87€

5Om10t 89€

5Om122t 89€

5Om122te 80€

adjustable beamsplitter mount of side drive 5Bm59t-1

5Bm69t-1 and 5Bm69t models


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Mirror / optics mount 5OM111 provides smooth and precise adjustment with sensitivity of 10 arcsec. it can be used as a tilt platform – with the spring clamp 4sc-28m4 and mounting post 3smp4-47. platform of the mount has a clear aperture of 6.2 mm in diameter.


mechanism kinematic

Drive type knob

adjustments Θx, Θy

special features platform mount

angular range ±10°


mounting thread m4 (2 holes)

Fine screw thread m6x35

Features:

• 10 arcsec sensitivity• high degree of versatility• miniature mounts for small optics

product iD price

5Om111 39€

5Om111-0 49€

5Om111-45 59€

5Om111-9s127h* 49€

5Om111-9s127h-0** 59€

* mount 5Om111 with 9s127h screws** mount 5Om111 with 9s127h screws and with adapter

5Om111a0

mirror / optics mount 5Om111

5Om111-0 5Om111-45 5Om111-9s127h-0

miniature precision mirror mounts

miniature precision mirror mounts ensure precise angular adjustments of small optics about two orthogonal axes with 10 arcsec sensitiv-ity. For mounting the m4 and m6 taped holes are provided. these black anodized aluminium mounts are ideal for holding of 25 mm and smaller optic in tight spaces.


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special positioners

Five-axis optical mounts consist of : side regulation two-axis kinematic mirror mount with two screws (thread pitch 250 µm (100tpi)), two-axis translation stage with 2mm travel range driv-en by two screws (thread pitch 250 µm (100tpi))ž, zZoom which provides 10mm travel range

Five-axis optical mounts hold 1-inch optics.


Optics diameter Ø25.4 mm

tilt/tip range ±2°

screw thread pitch 250 μm (100tpi)


XY translation range ±2 mm

screw thread pitch 250 μm (100tpi)

sensitivity for XY translation 1 μm

sensitivity for Z translation 1 μm

Z translation range 10 mm

material black anodized aluminium



Optics diameter Ø25.4mm

XY translation range ±2 mm

screw thread pitch 250 µm (100tpi)

sensitivity for XY translation 1µm

sensitivity for Z translation 1µm

Z translation range 10mm

material black anodized aluminium

Four axis kinematic optical mount 5KOm4-1

Five axis kinematic optical mount 5KOm5-1

Translation optical mount 5TOM accepts Ø25.4 mm optics.


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Y-Z positioner 5TLM-1 accepts Ø25.4 mm optics. Optics is stopped by a rest-flange inside the central aperture of the plat-form and is secured by a hex fixing screw with hard plastic tip. 5tLm-1 is ideal for microscope objectives, mounted pinholes, fiber optics chucks and diode lasers.

Features:

• travel range 3 mm• Fine adjustment screws with 0,25 mm pitch• the movable carriage could accept Ø25,4 optics up to 9mm

thickproduct iD Options price

5KOm5V-1 vacuum compatible mount 383€

5KOm4-1four-axis kinematic optical

mount257€

5KOm5-1five-axis kinematic optical

mount270€

5KOm5F-1 kinematic mount with

reinforced springs for heavy objects mounting

280€

5tOm2-1 two axis translation optical

mount: - XY translation range206€

5tOm3-1three translation optical

mount: - XY translation range; - Z translation range

213€

Y-Z positioner for lens, pinholes and objectives 5tLm-1two axis translation optical mount 5tOm2-1

Y-Z positioner for lens, pinholes and objectives 5ZYP are com-pact mounts designed to precisely position optical components in the plane orthogonal to the optical axis. ideal for microscope objectives, mounted pinholes, fiber optics chucks, and diode la-sers. the mounts provide 5 mm translation with sensitivity of 2 µm.


5tLm-1 25.4 119€

5tLm-1th* 25.4 119€*two plastic pading ring and retaining ring included


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Adjustable height platform 7VT173-25 of original design is a stable vertical translation stage of 25mm travel range. maximum load capacity – 3kg.a polished lead screw has 0.5 mm pitch. it allows defining the height of a platform with 20 µm sensitiv-ity. adjustable height platform is ideal for use with 7t173-50 or 8mt173-50 translation stages when it is necessary to define one or two horizontal coordinates at a certain height. the platform is produced from black anodized aluminium, the lead screw block is produced from stainless steel and bronze.

budget kinematic optical mounts

Budget kinematic optical mounts are designed for angular alignment of optical elements, in a range of 9° in both orthogo-nal axes. the tilting element is always true-kinematic registered. the mounts are produced of black anodized aluminium

product iD travel range, mm price

7Vt173-25 25 221€

product iD Details price

5ZYp-1-a1 positioner with ring a1 149€

5ZYp-1-B1 positioner with ring B1 149€

5ZYp-1-W0.8 positioner with ring W0.8 149€

5ZYp-2-a2 positioner with ring a2 159€

5ZYp-2-B2 positioner with ring B2 159€

adjustable height platform 7Vt173-25

product id Details price

5pm131-22 fine screws, mounting through

holes for m4(8-32) screws54€

5pm131-33 fine screws, mounting through

holes for m4(8-32) screws63€

5pm131m-22 fine screws, mounting through holes for m4(8-32) screws, right

hand version54€

5pm131m-33 fine screws, mounting through holes for m4(8-32) screws, right

hand version63€

Prism mount 5PM131 provides basic mounting for prisms, beamsplitter, cubes and etc. spring clamps 4sc series should be ordered separately.

prism/optics mount 5pm131

Y-Z positioner for Lens, pinholes and Objectives 5ZYp-2-B1


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multi-axis tilt platform provides angular and adjustment about two-axis - tilting and in-plane rotation. three angle prism / beamsplitter table provides non-calibrated tilt motion in three planes. it is the ideal work platform for prisms, beam splitters and mirrors, which needs to be precisely adjusted in angle about three orthogonal axes. a tilt / rotation stage provides two independent tilt adjustments within ±5° range and ±5° in-plane rotation adjustment.

Altechna offers two types of bases: kinematic and magnetic kinematic base which are used for repeated positioning of groups of units mounted on its platform.

Three angle prism / beamsplitter table 6TP169 provides non-calibrated tilt motion in three planes. it is ideal work platform for prisms, beam splitters and mirrors, which needed to be precisely adjusted in angle about three orthogonal axes.

product iD price

6pt110 170€

6pt169 196€

Tilt / rotation stage 6PT110 provides two independent tilt ad-justments within ±5° range and ±5° in-plane rotation adjust-ment. precision screws provide 9 arcsec resolution in rotation and both tilt planes. the mounting clamp with a spring-loaded disengagement knob allows easy insertion and removal of opti-cal components up to 39 mm height and 30×30 mm in square.

Base pOsitiOneRs

tilt/rotation stage 6pt110three angle prism/ beamsplitter table 6pt169


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Roll & Pitch Tilt Platform 7FA

travel in z axis -2 mm, +4 mm

travel roll, pitch +/- 4o

Resolution 10 arcsec

Multi-axis tilt platform 6TP116 provides angular adjustment about two-axis - tilting and in-plane rotation. the mounting platform is rotated around kinematic pivot point by two mi-crometers. the out-of-plane tilting range is ±2° and the in-plane rotation range is ±2.5°. two micrometers screws are located side by side for a handy use. the adjustment movements are not cali-brated, and they are uncoupled. the mounting platform has a 25 mm grid of tapped holes m6 and m4. two clearance holes Ø6.2 are provided in the base of the unit. this allows to attach 6tp116 to tables and breadboards.

Features:

• tilt platform• angular adjustment about two axes

product iD Dimensions, mm price

6tp116 148 x92 x33 188€

6tp115 148 x 70 x 33 188€

product iD price

7Fa3 189€

Roll & pitch tilt platform 7Fa3

multi-axis tilt platform 6tp116


tilt Θy ±2°

Rotation Θz ±2.5°

Load capacity 15 kg

Weight 1 kg


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tRansLatiOn & ROtatiOn staGes

Precision rotary stage 7R129 with a micrometer screw. Fine mo-tion range is 15° with resolution of 1 arcmin.


Rotation range

coarse 360°, resoliution 1°

fine 15°, resoliution 1arcmin

sensitivity 20arcsec

Reading accuracy 1arcmin

Wobble 1arcmin

Load capacity

horizontal 12kg

vertical 5kg

max drive torque 0.3kgm

product iD price

7R129 324€

7R129e 324€

polarizer holder 7R129

Rotation stage 7R150-1 main advantage of this precise rotation stage is that it has very compact dimensions and low-profile to-gether with the great aperture in the middle. this stage provides continuous rotation.

product iD aperture price

7R150-1 m27x1 339€

7R150-30 30 mm 343€

7R150e-1* m27x1 339€

7R150e-30* 30 mm 343€

* inch version

Features

• continuous rotation• Very compact design• no extra adapter plate• motorized version available

rotation stages

Rotation stage 7R150-1

motorized rotation stage 8mR151-1


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Rotation stage of big platform 7R171-200 is used to manually rotate large optical components through continuous 360° with accuracy of 1°, and finely to adjust the within 10° by a microm-eter, with accuracy of 0.5 arcmin. the stage has 50.8 mm clear aperture. the platform has a pattern of m6 mounting holes for components.


Rotation range

coarse 360°

fine 10°

Reading accuracy 0.5 arcmin

sensitivity 0.1 arcmin

Wobble 1 arcmin

Load capacity

horizontal 15kg

Mini rotation stage 7R7 provides smooth, low friction 360° rota-tion. a micrometer driving screw renders resolution 1’. a clear aperture of Ø 15 mm allows attachment of lenses and filters di-rectly in front of the stage. a removable ring (included) could be screwed into the aperture. “clear top” design allows attachment of larger components.


Rotation coarse/fine

range 360°/15°

resoliution 1°/1’

Load capacity

horizontal 5kg

Vertical 2 kg

product iD price

7R7 232€

7R7e 232€

Features

• Ø200 mm platform• 360° coarse rotation• 10° fine adjustment• Ø50.8 mm (2”) clear aperture

product iD price

7R171-200 399€

Rotation stage of big platform 7R171-200

mini rotation stage 7R7


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narrow translation stages

We offer various manual 1/2 axis translation stages with great travel range increased stability of precision. they come in various sizes from miniature to multi-axis assemblies. stages are made from steel or aluminum after that they are black anodized.

Translation stages 7T173 allow manual linear motion. a plat-form is spring preloaded against the driving screw to provide high resolution, low backlash, smooth and accurate motion. an array of mounting holes on a platform and on a base provide a variety of convenient mounting options, including mounting on 3mp series posts.


sensitivity 1 µm

tracking accuracy 2 µm

Reading accuracy 5 µm (1/2 division)

Load capacity :

horizontal 10 kg

Vertical 5 kg

product iD price

7t173-10 191€

7t173-20 224€

7t173-25 249€

2cp173-20* 15€

* connecting plate

Features

• 10, 20 mm travel ranges• Optional travel: 5, 6, 25, 30 mm• stackable for compact X-Y-Z configuration

translation stages 7t173

connecting plate 2cp173-20for stacking the narrow stages in X-Y motion


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low profile translation stages

Stable aluminium translation stages 7T68 have large mounting surface, great travel range for this relatively small size, low pro-file and increased stability of precision. Box designed reinforces the stage, reducing flex. the platform is preloaded by springs. the stage could be stacked immediately to other units or to their own type. Z-axis could be attached through angle bracket 2aB67-25-aL. the stage could be used upside-down. For imme-diate attachment the base has 2 clearance holes for m6 screws. micrometers 9s75m-25 comes as standard.


travel range 25 mm

sensitivity 1 µm

Reading accuracy 10 µm

angular deviation <200 µRad


Load capacity :

horizontal 20 kg

Vertical 5 kg

Features

• solid box design• 25 mm travel range• Large mounting surface• easily stacked in X-Y configuration• Right hand version 7t68-25tm available

stable aluminium translation stages 7t68

7t68-25 XYZ 3 axis translation system.


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Ball bearing translation stage 7T184-13 provides smooth, pre-cise single axis movement.

standards pecifications

Drive type side

travel range 13mm

sensitivity 1µm

angular deviation <200µrad

tracking accuracy 2µm

Reading accuracy 5µm (half division)

Load capacity

horizontal 10 kg

Vertical 3 kg

Popular translation stage 7T38 provides single axis movement.


travel range 15 mm

sensitivity 1 µm


scale graduation 10 µm

Load capacity

horizontal 10 kg

Vertical 5 kg

product iD price

7t38 234€

7t38XYZ 624€

Features

• micrometer drive• X-Y-Z configuration available

Features

• compact design• precise movement• 13 mm travel range• X-Y direct stacking• Lockable

product iD type price

7t68-25 standart stage 210€

7t68-25t side driven stage 217€

7t68-25tm side driven right handed 214€

7t68-25XYZ axis translation system 679€

7t184-13 - 220€

Ball bearing translation stage 7t184-13 popular translation stage 7t38

translation system 7t38XYZ


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XZ micro translation stage 7T228T provides smooth, precise two-axis movement. the driving screws are positioned so that the unit is controlled only from one side. that is why 7t228t is very handy in optical schemes with very dense placement of instruments. the travel of this stage is 4mm with sensitivity of 1 µm. to mount components on it, m2 tapped holes are provided. the unit has a clear aperture of 7mm in diameter. so it is ide-ally suited for use as a holder of diaphragms. the stage can be directly mounted on breadboards and other equipment. angle bracket 2aB128 may be used to combine the stage with other units.


travel range 4 mm

sensitivity 1 µm


Load capacity :

horizontal 0.3 kg

Vertical 0.1 kg

Features:

• Ultra compact configuration• precise rectilinear movement• 4mm X-Z or X-Y travel range• precision ball

product iD price

7t228t 220€

7t228tL* 235€

* Lockable version

XZ micro translation stage 7t228t

micro translation stages vertical positionersVertical stages 7VT40-13 is made in most compact design. plat-form is made with central m6 mounting hole and six m3 mount-ing holes for stacking with stages and other objects. Vernier scale is engraved on one side of the stage. travel range 13 mm.

3UBp-03 Universal base plate is required to fix stages to a flat surface e.g. optical table.


travel range 13 mm

sensitivity 1 µm


Reading accuracy 5 µm

Load capacity 5 kg

Features

• compact• high precision

product iD price

7Vt40-13 189€

3UBp-03 31€

Vertical stages 7Vt40-13


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dovetail linear translation stages

The dovetail translation stage 7T25-10 is miniature, ideal for use in applications where space is limited. the design uses a precision m4x0.25mm pitch lead screw for smooth linear posi-tioning along the entire range of travel. the moving platform is lockable. Various application accessories are also available.

standard pecifications

travel range 10 mm

Fine screw pitch 0,25 mm

sensitivity 1 µm

Drive location center drive

Bearings Dovetail

Load capacity 1,5 kg

Features

• compact design• Robust dovetail mechanism• Lockable moving platform• Rapid, smooth positioning• XY miniature dovetail stages

product iD application price

7t25-10X X axis 59€

7t25-10Y or Z axis

(addition to existing stage)59€

7t25-10XY YZ system 123€

7t25-10XYZ XYZ system 199€

2aB7t25-10 angle bracket 18€

3Bp7t25-10 Base plate 18€

dovetail translation stage 7t25-10


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mOtORiZeD pOsitiOneRs & cOntROLLeRstranslation stagesMotorized translation stages 8MT173 are created on the basis of 7t173 manual translation stages and have identical mechani-cal parameters. Resolution, speed and load capacity all depend on parameters of the motor, translation stages, as well as on the controller and driving mode a user chooses to use. For vertical (Z axis) mounting we offer angle bracket 2aB173-20.

two mechanical limit switches built into each translation stage used for emergency stop at ends of travel range or to establish a reference position with accuracy of several motor steps.

motor position can be visually determined with accuracy of one step by reading a scale engraved on dial knob fitted on motor shaft.

Body and platform of 8mt173 are made of black finished alumi-num. Functional parts are made of steel.


Lead screw pitch 0.25 mm

Resolution in full step* 1.25 µm

max. speed* 5 mm/s

Load capacity

horizontal 5 kg

Vertical 2 kg

Motorized linear stages 8MT175. Resolution of the motorized linear stages can be increased by using a step division function (up to 1/8 of the step) of our controllers. stages equipped with Dc or Dc for vacuum motors are available



Resolution in full step* 2.5 µm

max. speed* 10 mm/s

Load capacity

horizontal 8 kg

Vertical 3 kg

8MT50 motorized translation stages are compact design.


Lead screw pitch 1 mm

Resolution in full step* 5 µm

max. speed* 20 mm/s

Load capacity

horizontal 30 kg

Vertical 8 kg

motorized translation stages 8mt173motorized translation stages 8mt50


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Motorized translation stages 8MT167-25BS1 is designed for high-speed movement. Used ball bearing lead screw makes movement fast and smooth. the positioner also can be used with microscope on XY axles. as shown in the pictures, the up-per plate has a removable insert in the center, the size of which 2 inches, the base plate is made with slot size of 51 x 76 mm, on the same vertical. Linear motor positioning ssage provides high-resolution motion as well as high stability performance.

2AB175 - angle bracket for vertical mounting

3UBP175 - universal base plate for mounting on flat surfaces


Resolution in full step* 5 µm

max. speed* 25 mm/s

Repeatability 1.5 µm

Load capacity

horizontal 30 kg

Vertical 7 kg

Features:

• compact design• precise movement• X-Y-Z direct stacking• Lockable

Motorized translation stage 8MT184-13


travel range 13mm

Resolution 1.25 micron

Lead screw pitch 0.25mm

Weight 0.25 kg

Features

• narrow (30 mm)• compact design• high guide way accuracy

motorized translation stages 8mt167-25Bs1

motorized translation stage 8mt184-13


8mt173-20 20 402€

8mt173-30 10 439€

8mt175-50 50 786€

8mt175-150 150 1114€

8mt50-100 100 972€

8mt50-200 200 1630€

8mt167-25Bs1 25 565€

8mt184-13 13 490€

2aB175 - 68€

3UBp175 - 48€


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Motorized delay line 8MT160-300 provides precision path de-lays of up to 300 mm. Driven by a stepper motor with integrated limit switches, the motorized delay line offers a high-resolution delay of 2.5 µm. the main feature of this delay line are its high-stability, compact and monolithic design as well as high resolu-tion which makes the device ideal for integration in high preci-sion measurement systems. such delay line is in great demand in laboratories for precision optical path length control or other experiments (spectrum analysis, interferometry, etc.). motorized delay line can be controlled manually by means of dial knob with increments located on the end of the stage. this device also could be considered as a long travel (300 mm) motorized translation stage. Resolution could be improved by means of steps division in motor using our up-to-date stepper motor con-trollers.


travel range 300 mm

Resolution in full step 2.5 µm

Resolution in 1-8 step 0.31 µm

Load screw pitch 0.5 mm

max. speed 8 mm/s*

Load capacity

horizontal 10 kg

Vertical 3 kg



Resolution

Full step 2.5 µm

1/8 step 0.31 µm

max speed 10mm/sec

Load capacity

horizontal 50 kg

Vertical 6 kg

Motorized scanning stages 8MTF are designed for applications where high accuracy and repeatability is required. microscopy is the most common application for such devices. all scanning stages require a motion controller to operate.


8mt160-300 300 2490€

8mtF-75Ls05 75x75 1900€

8mtF-102Ls05 102x102 1990€

2aB175* - 68€

3UBp175** - 48€

* angle bracket for vertical mounting** Universal base plate for mounting on flat surfacesmotorized delay line 8mt160-300

motorized scanning stage 8mtF


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Motorized rotatory stages are used to finely rotate large optical and other components. top platform of the stage has a pattern of m6 and m4 mounting holes for mounting various components. clearance slots for m6 screws available on the bottom for fastening to opti-cal table.

Motorized rotary stage 8MR151 are series of rotation stages with integrated opto limit switch for home position reference.

For vertical mounting angle bracket 2VP150 available.

standard specifications:


Resoliution

in full step 0,6 arcmin

in 1/8 step 4.5 arcsec

Wobble 0,6 arcmin

Rotation speed 50°/s

eccentricity 10 µm

Load capacity :

horizontal 6,0 kg

Radial 1,7 kg

torque 0,5 n/m

Features

• motor 28• motors of other types are available.• inch versions available

motorized rotation stage 8mR151-1

rotation stages


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Motorized rotary stage 8MR190-2

8mR190-2-28 8mR190V-2-Vss42


Resolution in full step 0.6arcmin (0.01°)

max.rotation speed 8turn/min 2turn/min

Backlash 0

Wobble 0.5arcmin

eccentricity 10µm

Load capacity

horizontal 10kg

Vertical 2kg

torque 1nm 0.6nm

motorized rotation stage 8mR190-2-28

motorized rotatory stage 8mR191-28 (with full central hole)

motorized rotation stage vacuum version 8mR190V-2-Vss42. compatible with 10-6 torr vacuum.

Features

• high stability• Zero backlash• home/zero position limit switch• mounting modification available on request

Motorized rotary stage 8MR191

8mR191-28 8mR191V-Vss42


Resolution in full step 0.6arcmin (0.01°)

max.rotation speed 8 turn/min 2 turn/min

Backlash 0

Wobble 0.5arcmin

eccentricity 10µm

Load capacity

horizontal 10kg

Vertical 2kg

torque 1nm 0.6nm

Features

• three types of platform available: • without central hole (8mR191) • m27x1 for 1” optics mounting (8mR191-1) • Ø30mm aperture (8mR191-30)


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Large motorized rotation stage 8MRB250-152-59. to provide more usability, we are offering two modifications:

8MRB250-152-59 - motor is mounted on top of the stage.8MRB250-152-59D - motor is fixed to the bottom of the stage.


Belt drive 1:10

clear aperture 152,4 mm (6”)

Rotation range 360° continuous

Resolution

in full step 10,8’

in 1/8 step 81”

Repeatability

uni-directional 6’

bi- directional 15’

accuracy 15’

maximum speed 120 turn/min

Load capacity

axial 500 kg

radial 200 kg

torque 175 nm

Large motorized rotation stage 8mRB250-152-59

Features

• clear aperture 152,4 mm (6”)• extremely huge load capacity• Relatively compact• high speed• motor fixing on top and bottom

product iDaccepts optics,

mmprice

8mR151-1 25.4 687€

8mR151-30 30 697€

8mR190-2-28* 50.8 938€

8mR190-2-Vss42** 50.8 2379€

8mR191-28**** - 896€

8mR191V-Vss42**** - 2337€

8mRB250-152-59 152.4 3125€

8mRB250-152-59D 152.4 3125€

2Vp150 (for vertical mount-ing accessory)

29€

* Rotation stage with stepper motor 28 (0.67a, 200 steps)** Rotation stage with stepper vacuum motor Vss42*** Rotation stage with direct current (Dc) motor


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Universal motorized rotation stage 8mRU-1

a filter wheel version 8mRU-1Wa of universal rotation stage 8mRU. accepts up to eight 25.4 mm filters.

Universal motorized rotation stage 8MRU is a simple and du-rable low cost solution for use as optical element rotator, fil-ter wheel or universal rotating platform. center opening has a threaded m27x1 aperture for mounting 1” optical elements. Re-taining ring for fastening optics is included. 8mRU with various accessories can serve as several devices in one.


8mRU-1 25.4 655€

8mRU-1Wa 25.4 799€

8MRU-1 is a basic rotation stage that can rotate 25.4 mm optical elements.



Resolution

in full step 0.6°

in 1/8 step 4.5 arcmin

max. rotation speed 3÷5 rps

Wobble 2 arcmin

Reduction gear 3:1

Limit switches mechanical

Drive mechanism belt

Load capacity

horizontal 5 kg

Radial 1.5 kg

torque 4.5x10-3 nm


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motorized Z stage 8mVt70-13 motorized vertical translation stages 8mVt40-13

Compact motorized Z stage 8MVT70-13 of original design pro-vides 13 mm of reliable vertical motion. the stage ideally fits many motorized linear stages. 8mR151 series motorized rotation stages can be directly mounted on top of 8mVt70-13-1.


travel range 13 mm

Resolution in full step 5 μm

Resolution in 1/8 step 0.625 μm


maximum speed 20 mm/sec

Load capacity 4 kg

Unidirectional repeatability 1 μm

Bi-directional repeatability 2 μm

Motorized vertical translation stages 8MVT40-13 is made in most compact design. platform is made with central m6 mount-ing hole and six m3 mounting holes for stacking with 174 and 184 series stages and other objects. Vernier scale is engraved on one side of the stage. travel range 13 mm. Four m4 holes are made in the positioner ’s platform for mounting on other suit-able surfaces.


travel range, mm 13

Lead screw pitch, mm 1

Reduction gear ratio 1/60

Resolution*

in full step, µm 0.083

in 1/8 step, µm 0.01

max. speed*, mm/s 0.416

Load capacity, kg 6

vertical translation stages


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Motorized vertical lift stage8MVT120-5 offers precise vertical translation for elevating object up to 8 kg. an optional 1000-line rotary encoder is available for the stepper motor.


travel range 5 mm

Resolution

in full step 0,625 μm

in 1/8 step 0.078 μm

Lead screw pitch 0,5 mm

Wedge reduction rate 4:1

Repeatability 3 μm

accuracy 10 μm

Lift parallelism (to the base) 20 μm

mounting surface flatness 10 μm

position stability (max) 3 μm

maximum speed 2.5 mm/s

maximum load capacity 8 kg

Features

• high precision• high speed (up to 20 mm/sec)• compact design


8mVt70-13-1 13 950€

8mVt40-13 13 879€

8mVt120-5 5 1458€

8mVt100-25-1 25+1 1515€

Motorized vertical stages 8MVT100-25-1


travel range 25 + 1 mm

Resolution in full step 5 μm

Resolution in 1/8 step 0.625 μm


maximum speed 20 mm/sec

Load capacity 8 kg

Unidirectional repeatability 1 μm

Bi-directional repeatability 2 μm

Features

• compact• stiff and stable• two optical limit switches• clean room grease

motorized vertical lift stage 8mVt120-5

motorized vertical stages 8mVt100-25-1


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Motorized iris diaphragm mount8MID10-40 is designed for smallest diaphragm family.


closing speed (min to max) 1.2 seconds

stepper motor/gear 50:1

max aperture from 5mm up to 27 mm

min aperture from 0.5 mm up to 1.5 mm

Motorized iris diaphragm 8MID98-4-90 can be used in inacces-sible places or closed devices and controlled


Operation range Ø5 - 98 mm

Resolution

in full step 0.16 mm

in 1/8 step 0.02 mm

closing speed (min to max) 6 sec

Features

• smooth operation• swift operation• compact• adjustable inserts

motorized iris diaphragm mount8miD10-40

motorized iris diaphragm8miD98-4-90

in optics there are a lot of fields where accurate amount of light, precise projection, specific depth of focus and other requirements are necessary. For such areas the use of iris diaphragms is one of the best options.

iris diaphragms consist of leaves and case. Leaves are made of hardened spring steel. stainless chrome nickel steel can be used when better resistance to heat is necessary. the surface of leaves is polished and reducing the reflections. the edges of the leaves are rounded to achieve smooth operation. For increasing the slip of leaves an invisible coating is applied. next, protection from corrosion is guaran-teed by particular polishing process. Further, for producing the case, corrosion resistant aluminum alloy is used. Fine mat black look is achieved by black-anodizing the surface of the case.

motorized attenuators


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motorized screws and actuators

motorized mirror mounts

Motorized actuator 8CMA06


Resolution 1.25µm

Lead screw pitch 0.25mm

max.speed 6mm/s

nominal force 30n

Motorized mirror mounts 8MBM24 combines traditional 5mBm24 kinematic mirror/beamsplitter mount with motorized compact actuator. advantages motorized mirror mount: more precise positioning than with the manual adjusters, ideal for use in closed systems,integrated opto-electrical limit switches prevent damage, while providing homing - repeatability better than 10 arcsec.


travel range 4 mm

Resolution <1 arcsec

tilt range 9°(about two axes)

speed from 1 arcsec/sec to 1°/sec

Features

• clear edge Design• Kinematic• stable• mounting on either of 2 sides

product iD Optics mount, mm price

8mBm24-1-2* 25.4 699€

8mBm24-2-2* 50.8 731€

8mBm24-3-2* 76.2 776€

*with 2 motorized compact actuators

motorized actuator 8cma06

motorized mirror mounts 8mBm24

Features

• compact• high sensitivity• manual drive with knob• two limit switches


8cma06-13/15 13 300€

8cma06-25/15 25 349€


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Features

• compact design• annealed front panel• super stable with flat spring


8mKVDOm-1 25.4 688€

8mKVDOm-2 50.8 852€

Motorized vertical drive optical mount 8MKVDOM-1 is de-signed to minimize mount-induced wavefront distortions. in conventional mounts, the mirror is tightened by a side screw. Radial forces acting on the mirror induces parasitic wavefront distortion, such as astigmatism. 8mKVDOm-1 mirror mounts use secure 3-points mirror suspension in between frontal flat spring and the back plate. Uniformly distributed axial forces eliminate wavefront distortion.

Due thermal processes on optic holding part, all metal inner tensions were removed and part makes none micro movements.

specifications

tilt/tip range ±2,5°

sensitivity

by horizontal 3,8 arcsec. in full step of actuator

by vertical 3,9 arcsec. in full step of actuator in the middle tilt of platform

installed actuators 2 x 8cma20-8/15

travel range of actuator 6 mm

Resolution

in full step 1,25 μm

in 1/8 step 0,156 μm


Repeatability 1 μm

motorized vertical drive optical mount 8mKVDOm-1


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controllers

Microstep driver 8SMC1-USBhF (with UsB interface) comes with a suite of advanced software tools that can be utilized to control and adjust your stepping motors. all software tools op-erate on Windows 2000/Xp/Vista. smcView is a friendly, graphi-cal user interface for controlling, monitoring and adjustment of your stepping motors. it can also be used for easy setup to save and load of all parameters for each stepping motor. this inter-face supports up to 30 drivers simultaneously. UsmcDLL.dll is a dynamic link library for host programming in c/c++, Visual Basic and other languages. it includes all basic commands for step-ping motor control. some examples of these functions are also enclosed. smc.llb is a set of virtual instruments ( Vi) for national instruments LabView 7 programming language. some examples of these Vi’s are also included.

Users can connect to 8smc1-UsBhF various stepper motors us-ing “bipolar, two phase” connection. many motorized stages that can be driven by 8smc1-UsBhF: actuators, rotators, translators, variable wheel attenuators. these stages also can be mechani-cally fixed to various systems: XYZ translators, translators + rota-tor and others.

specifications

Electrical

• targeted for bipolar, two phase stepper motors with current ratings of 0.25a to 1.5 a. the current limit value is set by the manufacturer

• power supply voltage ranges from 12V to 36V• Overcurrent, overvoltage and temperature protection• synchronization input and Output• encoder inputs for stall detection (shared with synchroniza-

tion input)• Revolutions counter input (shared with synchronization input)

Motion

• Resolution: full step, 1/2, 1/4, 1/8• speed: 2-5000 steps/s• programmable speed and trip points• programmable acceleration and deceleration ramps• soft start/stop mode

Control

• pc control via UsB interface• Optional handheld remote offers manual two button direc-

tional control• additional features include two programmable limit switches,

an emergency limit switch, encoder, and revolution sensor for stall detection and input/output for synchronization

Programming

• Graphical user interface smcView for Windows 2000/Xp/Vista• Drivers and dynamic link library for Windows 2000/Xp/Vista/

mobile host programming• set of virtual instruments for national instruments LabView

Mechanical

• Rohs compliant• Operating temperature range: 0 to 70°c• Box size for 1-axis controller : 90 x 120 x 70 mm (B1)• Box size for 2 and more axis controller : 180 x 120 x 90 mm (B2)


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product iD Details price

8smc1-UsBhF-B1-1 1 axis controller 320€




attenUatORs

Variable wheel attenuator 10WA168 is a basic model with 4 fil-ter-set wheels. each wheel contains 4 filter mounts each of Ø20 mm with clear aperture of Ø18 mm. each filter mount is inclined by 4°to avoid retroreflections. each wheel has 4 fixed positions.

product iD Filters price

10cWa168 3 (+1 empty space) 549€

10Wa168-1 16 (not included) 297€

10Wa168-1-2 8 (not included) 210€

Close variable wheel attenuator 10CWA168 is used when it is necessary to fully eliminate the side background lighting when using photodetectors with high sensitivity

Variable wheel attenuators 10Wa168 &10cWa168

SERVICES & OPTICAL MATERIALS

METROLOGY TESTS 256

MEASUREMENT SETUPS 258

LASER AND NONLINEAR CRYSTAL REPOLISHING SERVICES

261

OPTICAL MATERIALS 262


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METROLOGY TESTSDescription

Altechna is concerned about your success in experiments and final product performance, therefore our qualified metrology laboratory in cooperation with Vilnius University and other Lithuanian science institutes is offering variety of laser optics quality tests:

• Opticalsurfacequalitymeasurements;• Transmittanceandreflectancemeasurementsin190-1100nmandin1100nmto20000nmrange;

• Surface flatness, wavefront distortion measurements of flatandsphericaloptics;

• Anglemeasurementsforprisms,wedgesandotheroptics;• Non-contactROC,Focallengthmeasurements;• LaserInducedDamageThreshold(LIDT )testsforwiderangeoflaserwavelengths;

• Opticalabsorptiontests;• Totalscatteringmeasurements;• Custommadetests.

Interferometer

For accurate metrology of surface form for flat and sphericalsurfaces we are using ZYGO Verifire XP/D Phase Shifting interferometer. Variety of accessories allows to our engineers to measure coated and uncoated optics, radius metrology allows us to test spherical surfaces for form irregualities and Radius of Curvaturewithradiusof±20-±800mm.Forpolarizationsensitiveoptics,suchaslasercrystals,linearpolarizationoptionisused.

InterferometerVerifireXP/D,(Zygo)

Lens testing

Non-contactand lessdamagingmethod isused for lens radiusof curvature, focal length and centration measurements. Air bearing stage and electronic collimator allows to reach less than 0.1 μm accuracy when measuring centering errors. Additionalaccessories extend our capabilities to measure focal length valuesupto±5meters,ROC–±800mm.

GoniometerGoniomatHR,(Moeller-WedelOpticalGmbH)

OptiCentricMOTwithOptiSphericmodule,( Trioptics)

Goniometer

High accuracy goniometer with air bearing rotary table allows to measure angles for prisms, polygons, wedges and plano opticswithaccuracybetterthan0.6acrsec.Developedsoftwarekit allows to determine refraction indices to identify glass types.


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Measurements by product group

Product Measured parameterSubstrates

Non-linearandlasercrystalsPrismsWedges

Surface qualityDimensionsFlatness

Transmitted wavefront distortionParallelism, angles

Dielectric coated opticsMetallic coated opticsNon-polarizingcubes

Filters

Surface qualityDimensions

SpectraFlatness

Transmitted wavefront distortionParallelism

PolarizingcubesPolarizers

Surface qualityDimensions

SpectraforsandppolarizationsFlatness

Transmitted wavefront distortionLenses Surface quality

DimensionsRadius of CurvatureEffectiveFocalLength

IrregularityPower

WavefrontdistortionCentration

Waveplates Surface qualityDimensions

ContrastAxicons Surface quality

DimensionsBessel beam in near and far field

Lasers(DPSS,gas) Power stabilityBeam profile

SetofCWlasers(532nm,632.8nm,800nm,1030nm,1064nm)

SpectrophotometerSpecord200,(AnalyticJena)

StereomicroscopeSZX7-0,75x-100xAnalyticalmicroscopeBX51TRF,5x-100x(Olympus)


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MEASUREMENT SETUPS

Setupforpolarizationsensitiveelementstransmissiontest.

Setup for AR coated windows, lenses, mirrors, waveplates or other surfaces reflection test. Test angle can vary from close to zero degrees. Reflectance also can be measured inspectrophotometer with reflectance module at fixed 5 degrees angle.

Setupforwaveplates(λ/2,λ/4)test.

Setup for axicon quality test. Screen is used for visual ring inspection, CCD – for Bessel beam profiling.

Measurement setup for distortion of a plane wave transmitted through windows, filters, and prisms.

Measurement setup for surface flatness of plano elements such as mirrors, prisms, and windows. This setup also is used for parallelism measurement of transparent materials.

If Transmission sphere is used instead Transmission flat, convex or concave spherical surfaces could be examined for surface figure and irregularity.


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Autocollimator Air bearing rotation table

AutocollimatorEFLTest sampleLight source

AutocollimatorRorating test sampleLight source

Autocollimator ROC Test sample

Goniometer is used for wedged windows, prisms angle, pyramidal error measurements.

Non-contactmethodisusedforRadiusofCurvatureforconvexand concave lens measurements. Cylindrical lens is also tested with this setup.

Non-contact method is used for Effective Focal Lenght, BackFocal Lenght, MTF function for convex and concave lensmeasurements.

Lens centration errors are measured by rotating sample over it‘s axis. Measurements are performed either in reflection or in transmission modes.


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PRICE LIST

Test Description

Price per sample, Euro*

1 Visualinspection(cleaning,photo)

Visualy elements are inspected under white light source, special and soft paper is used forcleaning.Stereomicroscopesforsmalldefectvisualizationisused,defectsalwaysarerecorded by camera and included into test report.

5

2 Transmittance and reflec-tance,190-2500nm

TransmittanceandreflectanceismeasuredwithSpecord200intherange190-1100nmTransmittanceintherange1000-3300nmismeasuredwithShimadzuinstrument

15

3 Transmittance and reflec-tance,2500-20000nm

Transmittanceandreflectanceintherange2500-20000nmismeasuredwithThermoscietificFTIRspectrometer.

30

4 ROC(5-800)Focallength(5-5000)

Lens parameters such as efective focal lenght, radius of curvature, back focal lenght, also dublets centration is measured by non contact method with combination of Opticentric and OptiSpheric instruments.

30

5 ROC(30-800mm)

ForinterferometricmeasurementsweuseZYGOXP/ZFizeuinterferometer.Accesories,such as transmission flats, transmission spheres and attenuator allows to to measure flatness/irregularity, wavefront distortion in transmittance for plano and spherical optics. Integrated digital radius scale is used for Radius of Curvature measurements with accuracy betterthan0.1mm.Selectionoftransmissionspheresallowstomeasurebothpositiveandnegativelenses.SoftwaregivesvaluesofZernikecoeficients(aberations),modulationtransfere function, difraction data of the lenses.

40

6 Flatness,wavefrontdistor-tion for plano/plano optics

30

7 Surface irregularity, wave-front distortion for spherical optics

40

8 Angle, wedge Wedges,prismandpolygonanglesaremeasuredwithgoniometerGoniomatHRwithinaccuracyof0.6arcsec.

20

9 Laser induced damage threshold

Laser induced damage threshold could be measured with femtosecond or nanosecond pulsed lasers.All measurements for “1 on 1” and “S on 1” procedures are performed according to ISO 11254standards.Followingoptionsareavailable:1064,532,353nm,3-5ns,1-10Hz1030,515,343nm,200-400fs,1kHz–200kHz

300-450

10 Preparation, engineering for non-standardtests

Fornon-standardtestweusefollowingCWlasersources:1030nm,max.power800mW,stability<3%1064nm,power200mW,stability<3%532nm,max.power500mW,stability<3%632.8nm,power3mW,stability<1%800nm,power500mW,stability<3%

30/hr.

11 Packing and Labeling Vacuuming or packaging in plastic, membrane boxes with optional company logo print On request


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Polishing of the crystals

Crystals after polishing

LASER AND NONLINEAR CRYSTAL REPOLISHING AND RECOATING SERVICES

ALTECHNA is capable to repolish and coat most of existing laser and nonlinear crystals, including:

1. Nd:YAG2. Ti:Sapphire3.KTP4.KDP/DKDP5. ZnGeP

2

6. AgGaS2/AgGaSe

2

Services include drilling, cutting, re-polishing and coating.Altechna also can provide wedged ends or tilted ends for the elements. Most of the anti-reflection, high reflecting or partial reflectinglaser line dielectric coatings can be applied on the repolished elements. Read more about Recoating at the Coatings Section (page83-95)

Description

Parallism error ≤10arcseconds

Perpendicularity ≤5 arc minutes

Surface quality 10-5Scratch&Digs(perMIL-O-13830A)

Suface flatness <λ/[email protected]

Dimensional tolerances Diameter:+0.00/-0.05mm; Length:±0.5mm; Chamfer:<0.1mm@45º

Clear aperture Central95%

Standard refurbishing specifications

You are welcome to contact our engineers for assistance with your custom requirements!


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OPTICAL MATERIALS

ALTECHNA offers a broad range of materials for various optical applications, suited for a wide range of customer goods as well as for industrial and scientific applications. Our range of optical glasses includes suchpopularmaterials as BK7,CaF

2, Sapphire,

Fused Silica, MgF2, Zinc Selenide Laser Grade, Calcite, Crystal

Quartz and other infrared and ultraviolet materials. These areonly examples and a small fragment of our capabilities. There are two instances in which you might need to know more about optical materials. First, you may need to determine theperformance of a catalog component in a particular application. Second, you may need specific information when selecting the material for a custom component. The data in the following is intended to assist in these situations.

Description

Optical Materials

Materials Refractive index “Density(g/m3)”Thermal expansion coefficient(10-6/K)

BK7 1.5164(588nm) 0.330-2.1 2.51 7.5

SF11 1.78472(588nm) 0.370-2.5 4.74 6.8

F2 1.62004(588nm) 0.420-2.0 3.61 8.2

FusedSilica 1.4858(308nm) 0.185-2.5 2.20 0.55

CaF2 1.399(5.0mm) 0.170-7.8 3.18 18.85

BAF2 1.460(3.0um) 0.15-12.0 4.88 18.4

Sapphire 1.755(1.0mm) 0.180-4.5 3.98 8.4

Silicon 3.4179(10mm) 1.200-7.0 2.33 4.15

Ge 4.003(10mm) 1.900-16 5.33 6.1

ZnSe 2.40(10mm) 0.630-18 5.27 7.8

ZnS 2.2(10mm) 0.380-14 4.09 6.5

LiF 1.39(500nm) 0.150-5.2 2.64 37

KBr 1.526(10mm) 0.280-22 2.75 43

MgF2 no=1.3836ne=1.3957(405nm) 0.130-7.0 7.37 a:13.7b:8.48

YVO4 no=1.9500ne=2.1554(1.3mm) 0.400-5.0 4.22 a:4.46b:11.37

Calcite no=1.6557ne=1.4852(633nm) 0.210-2.3 2.75 a:24.39b:5.68

Quartz no=1.5427ne=1.5518(633nm) 0.200-2.3 2.65 7.07

a-BBO no=1.6749ne=15555(532nm) 0.190-3.5 3.85 a:4.0c:36

LiNbO3 no=2.2863ne=2.2027(633nm) 0.370-4.5 4.64 a:16.7c:2.0

Workshop of photonics

coMpAnY profiLE 264

fEAsiBiLitY stUDY on LAsEr MicroMAchininG

264

LAsEr procEss DEVELopMEnt 265

sMALL scALE proDUction 265

cUstoM LAsEr sYstEMs for LABorAtorY 266

•femtoLAB 266

•soLLAs 267

•nscULptor 267

DEVELopMEnt of inDUstriAL LAsEr MA-chinEs

268

•femtofAB 268

softWArE for LAsEr MicroMAchininG 269

fEMtosEconD LAsEr MicroMAchininG 270

•samples of femtosecond micromachining technology

271

MULtiphoton poLYMEriZAtion tEchnoLoGY

279

•Mpp applications 281

iLLUstrAtions soUrcE 283

/ www.wophotonics.com264

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coMpAnY profiLE

cooperation with our customers usually starts with a need to perform a specific micromachining task. the complexity of the task may depend on the material, type of fabrication, speed of processing and other requirements.

the first step is usually a feasibility study, which indicates whether lasers are capable to perform the task. if it is a “yes”, then the customer decides how far to go down the steps of cooperation with Workshop of Photonics:

1. feasibilty study

3. Design of a system/module

custom laser systemsfor science

Laser Machines for industry*

Warranty & support

2. Laser process development(laboratory prototype)

small scale production

* in partnership with manufacturing machinery producers

fEAsiBiLitY stUDY on LAsEr MicroMAchininG

need to fabricate micron scale structures on the surface or in the bulk? Already tried and disappointed with other technologies? our laboratories equipped with ultra-short pulse lasers (from below 300 femtoseconds) is a place where machining perfection can be achieved.

our researchers will test your materials to achieve desired fabrication mode and consult on implementation of it in mass production. our working experience covers great variety of materials and our original micromachining software scA allows achieving the desired results fast.

results of a feasibility study:

• principle answer if laser can be used to achieve results desired by the customer

• Laser parameters, at which the result is achieved (optional)

www.wophotonics.com / 265Ge

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LAsEr procEss DEVELopMEnt

sMALL scALE proDUction

since micromachining workstations incorporating ultra-short pulse lasers is a significant investment, it is not always worth, it is not always worth buying one. Especially if you need to machine a small batch of articles, consider using our job shop services.

Most of laser micromachining applications are not as straightforward as for example marking. some processes need development which takes weeks and even months. not only different laser parameters have to be tested but also various beam shaping and focussing solutions.

A typical approach for comprehensive process development contains following steps:

• testing of different wavelengths in order to explore light-matter interaction

• testing of different focusing optics• selecting and testing the most suitable positioning solution• determining, what’s required for repeatability and required

speed of process• optimising software functionality for convenient process

control

You are welcome to contact us with specific micromachining tasks. We are committed to develop a micromachining process for you. if a task is more demanding, we are ready to involve our academic partners in search of a solution.


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cUstoM LAsEr sYstEMs for LABorAtorY

Every laboratory has specific applications and every scientist has its own approach. Workshop of photonics develops customized laser systems for your laboratory, so you get what YoU need and onLY what you need.

Based on our partners’ and our own know-how in laser micromachining laser micromachining, we will select appropriate configuration to meet your specific requirements.

• Laser source• sample positioning system• Beam delivery and scanning unit• Laser power and polarization control• software for system control• Machine vision • sample holders and special mechanics• Dust suction unit• other devices

We will provide a cost-effective solution for your laboratory. A proven flexibility of femtoLAB concept will allow you to further expand and upgrade your system when new requirements arise or budget becomes available.

femtosecond laser micromachining system for scientific laboratories. Equipped with nanometer accuracy and resolution linear positioning stages, high performance galvanometer scanners and versatile micromachining software scA, femtoLAB becomes an entire laser laboratory on an optical table.

tunable parameters

• pulse duration (<160 fs – 10 ps);• repetition rate (1 – 1000 khz);• Average power (up to 15W );• Wavelengths (1030, 515, 343, 258 nm).

femtoLAB

* for purchase contact [email protected]


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soLLAs

An industrial-research laser machine for c-si solar cells. Equipped with cutting edge duet – femtosecond UV laser and nanosecond ir laser, sollas is a multi-tasking system, designed for industrial research or up to 3 MW/a capacity pilot manufacturing lines.

features

• optimized for 2.5 MW/a throughput industrial-research line• femtosecond UV and nanosecond ir laser sources• Machine vision system detecting rotation and adjusting laser

scanning field• precise laser beam control in space using high-performance

galvanometer scanners 5’’ and 6’’ wafer processing• intuitive touch-screen user interface for simple production

mode operation (scA engineer)• full functionality software access in research mode (scA

engineer)

sollas performs 4 technological processes

• selective sinx/sio2 removal• Back contact laser firing• Edge isolation• Laser marking• other processes are integrated after feasibility tests

nscULptor

nscULptor is a turnkey 3D laser lithography system for fabrication of nano structures. operation of the system is based on multi photon polymerization (Mpp) technique and works with many conventional photoresists available in the market. nscULptor enables prototyping and production of various three dimensional structures at nanometer accuracy and resolution.

All processes of fabrication are integrated into a single system

• 3D model creation and preparation• Direct laser writing• post-processing

Advantages

• All-in-one solution• 100 nm – 10 μm resolution• complex 3D objects• Variety of polymers• small footprint


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DEVELopMEnt of inDUstriAL LAsEr MAchinEs

needs of industrial customers are rather different from those of an academic laboratory: speed, repeatability and efficiency are in focus. therefore our laser solution usually is a part of a bigger manufacturing machine or production line. Usually it is built by specialized integrators or producers of manufacturing machinery.

knowing your application of laser micromachining and process needed to implement it, Workshop of photonics will develop a specific task optimized laser machine. system configuration will be selected to assure quality, speed and reliability of execution of your task. We will select the needed hardware components including:

• Laser source• sample positioning system• Beam delivery and scanning unit• Laser power and polarization control• software for process control• Machine vision and sample recognition• sample holders and special mechanics• Dust suction • other devices

in order to automate the fabrication process, a custom adaptation of our laser micromachining software scA engineer can be designed (see page 11). this will not only speed up the fabrication process, but will also reduce participation of an operator to the very minimum. on the other hand, high-level users will have a special interface to configure the process or add new tasks.

Usually we offer our services to laser system integrators and producers of manufacturing machinery. however through cooperation with our partners, we can also deliver complete laser machines ready to install at your production site.

femtofAB

features

• high fabrication speed – up to 350 000 px/s• fabrication of difficult objects with submicron resolution• Minimal heat affected zone in femtosecond micromachining

mode• Aerotech based precise object positioning with submicron

accuracy• precise laser beam control in space using high-performance

galvanometer scanners• shot number control (single to 350 khz)• synchronization of laser pulses with moving object in space

and time domains• original software interface for control of all integrated

hardware devices

More information at http://www.wophotonics.com/products/

femtofAB is a turnkey femtosecond laser machine for industrial use. configuration is selected and carefully tuned according to a specific laser micromachining application, including laser cutting, laser scribing, laser drilling and 3D laser milling with any desirable material (with >2,4 GW peak power). system is protected by class 1 equivalent laser safety enclosure and is controlled through a single scA engineer software window.


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softWArE for LAsEr MicroMAchininG - scA

scA software was created to provide speed, flexibility and visibility to laser operators. it makes micromachining tasks easy to describe, fine-tune and repeat. key benefits of the software:

• the software eliminates the need to work with G-code completely

• WYsiWYG interface• convenience in entering algorithms and mathematical

commands• fast and easy to correct, fine-tune and then repeat machining

task • Directly a wide range of equipment• customizable to fit special requirement of scientific or

industrial applications

the software comes in two versions:

• Dedicated primarily to scientists to be used in their research.

• complete functionality• Machining rich in functions

and options • Live sample view through

camera• complex machining tasks

for laboratory -

• Designed for industrial applications. it is meant for machinery integrators and end-users of laser machines.

• task optimized functionality

• Machining as simple as required

• custom user interface• Edge detection, marking

recognition• Long term stability

for industry -

core functionality embedded in both scA versions:

• Direct control of hardware starting with laser, positioning stages, galvanometric scanners and going to power attenuators and power meters, polarization rotators, machine vision, special i/o and other peripheral devices.

• DXf, pLt, stL, BMp file import• import of data from tXt or XML files• Digital and analog i/o control• fabrication preview window• camera view calibrated with fabrication preview• Machine vision module for sample detection

.stl file sliced by scA professor

sliced object, having 3 shells to thicken the wall


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our competences, accumulated know-how and well equipped laboratories are capable to perform these processes:

• precise drilling, cutting, dicing and making• Ablation, etching, 2.5 D milling• 3D in bulk engraving• surface micro-nano structuring• Laser-induced Backside Wet Etching (LiBWE)• refractive index modification in transparent materials• optical micro-manipulation• two-photon polymerization

femtosecond laser micro fabrication is currently the most precise technological platform among other laser technologies, which is used for material processing. first ofall, femtosecond laser pulses distinguish itself as causing minimal heat effect, therefore almost any solid state material can be fabricated with submicron resolution.

fEMtosEconD LAsEr MicroMAchininG

Workshop of photonics is developing microfabrication technological platform, in order to provide scientific and industrial customers with:

• feasibility studies• fabrication process development• small scale production• Micromachining system development or mass production.• Laboratory rent and demo

* More information athttp://www.wophotonics.com/applications/


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Processing of solar cells

Applications:

• front contact formation• Back contact formation

Edge isolation for solar cells

selective dielectric layers removal for solar cells

Laser marking of solar cells

sAMpLEs of fEMtosEconD MicroMAchininG tEchnoLoGY

10 μm

50 μm

50 μm

53,591 μm 88,611 μm


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Nano ripples

• Up to 200 nm ripple period fabricated using ultra-short laser pulses

• individual nano-feature size on ripples: 10 – 50 nm• controlled period, duty cycle and aspect ratio of the ripples

Application:

• Detection of materials with increased sensitivity using surface-enhanced raman scattering (sErs)

• Bio-sensing, water contamination monitoring , explosive detection etc.

1 μm

Developed in cooperation withswinburne University, Australia

Marking of contact lens

• Marking made inside a bulk of contact lens, preserving surface of lens and distortions

• Exact positioning of markings – 3D text format

Application:

• product counterfeit protection • Development of novel products

100 μm

Metal micromachining

• 3D structures formed on steel surface• high precision and surface smoothnessachieved

100 μm


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Selective metal coating ablation (removal)

• selective ablation of metal coatings from various surfaces• Depth and geometry of ablation may vary

Application:

• Lithography mask production• Beam shaping elements• optical apertures• other

10 μm

titan coating selective ablation

Apperture array fabrication Gold layer removal without damage to Mgo substrate – Au layer removal without

damaging

chrome ablation for beam shaping

Amplitude grating formation

chrome ablation from glass substrate

50 μm 50 μm

Texturized sapphire surface

• Micron resolution• Large area processing• single pulses used to form craters on the

surface

Application:

• Better light extraction in LED • semiconductor structure growth

30 μm 10 μm


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Processing of optical fiber

• All types of fiber can be processed• hole diametre<10 µm• no impact on fiber strength• no undesired surface damage

10 μm

Drilling

Drilling to the middlescattering

50 μm100 μm

optical fiber

Glasssapphire

Marking inside a bulk of transparent material

• colorful structures due to small pixel size• surface not affected• Very small or no cracks near markings• Low influence on strength of the substrate

100 μm


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Metal hair

Marking, patterning capabilities:

• smallest spots up to 3 µm in width• Micron level positioning• no heat effect

Glass holes

• Various hole sizes with routine tapper angle better than 5 deg

• Minimal debris around the edges of holes

Application:

• Microfluidics

top view cross-section

100 μm

Stent cutting

• holes in stent wall, cross-section view• polymer stent• no heat effect, no debris• Minimal taper effect

Application:

• Vascular surgery

100 μm 100 μm


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Optical fiber lensed using MPP technique

• Matching refractive index• shape flexibility• resolution from 100 nm to 20 μm

Applications:

• Medical fibers• fiber collimators

200 μm

Diamond cutting

• Low carbonization• no hAZ• Low material loss

Applications:

• Diamond sheet cutting• Diamond texturing/patterning

100 μm

Micro channel formation

• Wide range of materials – from glass to polymers

Applications:

• Microfluidic sensors• Waveguides

25 μm

3 μm

> <


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Steel foil μ-drilling

• no melting• Micron diameter

Applications:

• filters• functional surfaces

10 μm

Ferroelectric ceramics etching

• no or low melting• Easily removable debris• Good structuring quality

Applications

• infrared sensors for cameras• Memory chips

20 μm

Silicon laser assisted etching

• no hAZ• no melting

Applications:

• solar cell production• semiconductor industry

30 μm


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Glass tube drilling

• controlled damage and depth

Applications:

• tissue biopsy equipment

20 μm

15 μm

Hologram production

• Example: hologram view generated using glass sample

100 mm

Mask for beam splitter pattern deposition

• Borosillicate glass• 150 um thickness• ~900 holes per mask• Mask diameter 25,4mm

Appplication:

• selective coating


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MULtiphoton poLYMEriZAtion tEchnoLoGY

the scA laser automation software product family is distinguished among other existing laser software solutions by the key working principle – it controls positioning stages by directly addressing the command libraries of the positioning stages software (no machine code conversion). structures of any geometry can be fabricated directly from cAD file. there are no limitations for object shape or direct writing geometry, except those limited by obvious laws of physics.

photoresist polymer materials

• Variety of photoresist materials with required features can be chosen;

• no structural distortions;• certain wavelength absorption;• refractive index matching.

Multiphoton polymerization is a unique technology for 3D structuring of micron scale objects with nanometer precision. femtosecond laser beam is focused inside a drop of sol-gel or other types of photoresistive polymer and desired pattern is “written” precisely point–by-point (fig. 1 a and b). then, the unsolidified remainder of the photoresist is washed away leaving only the fabricated microstructures on the substrate.

features

• 100 nm – 10 μm writing resolution• Medium cost per sample• Variety of polymers• complex 3D objects

What is a “technological platform”?

Mpp technological platform can offer a flexible solution for micro prototyping and production. it is a combination of feasibility studies, small-scale production and developmentof turn-key workstations. this platform includes certain steps from selecting the most suitable photoresist to building task-dedicated laser system for science or industry.

how does Mpp Work? Laser system software “scA”

*1


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20 μm

standard direct writing is able to make repeatable structures as small as 100nm, though by employing self-polymerization effect, the smallest lines can be around 20 nm. this effect occurs when certain distance between polymerized structure walls is kept, so self-polymerizing structures can be controlled, at least to some extent.

> < 90nm

repeatability

reliable and multifunctional software ‘scA professor ’ensures fast preparation, stable workflow. 3D lithography is related to huge amounts of data, which has to be transmitted between computer and positioning controllers. Many systems crash because of poor software adaptation to these specific tasks. ‘scA professor ’ splits the data in portions to deliver them safely and timely to the controllers. Moreover, identical structures can be fabricated by direct laser writing process but in order to save time and work for large area patterning stamping technique can be used.

Main applications

• Microoptics• photonic crystals• regenerative medicine

5 μm

10 μm

precision and controllable self-polymerization

*3

*4

*5



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Mpp AppLicAtions

Application in photonics

highly repeatable and stable technological process aims at fabrication of detractive gratings and photonic crystals.

Application in micro optics

Many polymers are transparent to visible light and can be combined with other materials like Zn or Ge. the ability to control light flow can be used in micro optical devices, such as micro lenses, hybrid micro lenses with a phase gratings, micro lens arrays, vortex beam screw generators, vortex generator arrays or other. the Mpp technology allows fixing of such micro optical devices on limited surfaces like the tip of an optical fiber.

Application in regenerative medicine

regenerative medicine is the most promising application field for Mpp technology, because polymerization can offer variety of custom elements which need controllable precision, biocompatibility or biodegradability. polymeric scaffolds for stem cells growth can be fabricated in any 3D shape for application in tissue engineering.

*6 *7

*8 *9

*10

*11 *12

*13 *14

10 μm 15 μm 20 μm 20 μm


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• scaffolds for tissue engineering.the last picture shows that artificial scaffold ambient is suitable for cell proliferation, because there is a cell growing in mitosis stage.

• Biocompatibility and biodegradability have been tested in vivo and in vitro. histological tests show that sol-gel material is more biocompatible that a surgical suture or surgical clip.

if you are interested in two-photon polymerization technological platform do not hesitate to contact us, we would gladly answer to your questions and give you the best solution according to your specific requirements.

*15

1.32 μm ><

*16

3.2 μm>< 36 μm

*1727 μm

3.5 μm

100 μm

*18

27 μm

*19 *20

30 μm 5 μm

*21

mitosis



1, 3. Mangirdas Malinauskas, Arune Gaidukeviciute, Vytau-tas purlys, Albertas Zukauskas “Direct laser writing of mi-crooptical structures using a Ge-containing hybrid material” Metamaterials 5 (2011) 135–140

2. Mangirdas Malinauskas, holger Gilbergs, Albertas Zukauskas, Vytautas purlys, Domas paipulas, roaldas Gadonas, “A femtosec-ond laser-induced two-photonphotopolymerization technique for structuring microlenses” J. opt. 12 (2010) 035204 (8pp)

4, 5. M. Malinauskas, V. purlys, M. rutkauskas, A. Gaidukeviciute, r. Gadonas “femtosecond Visible Light induced two-photon photopolymerization for 3d Micro/nanostructuring in photore-sists And photopolymers” Lithuanian Journal of physics, Vol. 50, no. 2, pp. 201–207 (2010)

6, 7. Mangirdas Malinauskas, Albertas Zukauskas, Vytautas purlys, kastytis Belazaras, Andrej Momot, Domas paipulas, roaldas Ga-donas, Algis piskarskas, “femtosecond laser polymerization of hybrid/integrated micro-optical elements and their character-ization” J. 2010 J. opt. 12 124010

8, 9, 10. Etienne Brasselet, Mangirdas Malinauskas, Albertas Zukauskas, saulius Juodkazis photo - polymerized microscop-ic vortex beam generators: precise delivery of optical orbital angular momentum Appl. phys. Lett. 97, 211108 (2010); doi: 10.1063/1.3517519

11, 12. Mangirdas Malinauskas, holger Gilbergs, Vytautas purlys, Albertas Žukauskas, Marius rutkauskas and roaldas Gadonas, “femtosecond laser-induced two-photon photopolymerization for structuring of micro-optical and photonic devices” proc. of spiE Vol. 7366 736622-1 (2009)

13, 14, 15, 16. M. Malinauskas, p. Danilevicius, D. Baltriukiene, M. rutkauskas, A. Žukauskas, Ž. kairyte, G. Bickauskaite, V. purlys, D. paipulas,V. Bukelskiene, r. Gadonas “3d Artificial polymeric scaffolds for stem cell Growth fabricated By femtosecond La-ser” Lithuanian Journal of physics, Vol. 50, no. 1, pp. 75–82 (2010)

17, 18, 19, 20. M. Malinauskas, p. Danilevicius1, A. Zukauskas1, G. Bickauskaite, V. purlys, M. rutkauskas, t. Gertus, D. paipulas1, J. Matukaite, A. kraniauskas, r. sirmenis, D. Baltriukiene, V. Bukel-skiene, r. Gadonas, V. sirvydis, A. piskarskas “Laser 3D Micro/nanofabrication of polymers for tissue Engineering Applica-tions” Latvian Journal of physics And technical sciences 2011, nr. 2

21. M. Malinauskas, p. Danilevicius, A. Zukauskas, D. paipulas, V. purlys, r. Gadonas, A.piskarskas D. Baltriukiene, r. Jarasiene, V. Bukelskiene, A. kraniauskas, r. sirmenis, V. sirvydis. “Biocom-patibility of polymers and laser-fabricated three-dimensional microstructured polymeric scaffolds for biomedical applica-tions” submitted for “Engineering in Life sciences” journal oc-tober 11, 2010

* iLLUstrAtions soUrcE

Mokslininkų st. 6A, 08412 Vilnius, LithuaniaPhone:+37052725738•Fax:+37052723704

[email protected]•www.altechna.com

Altechna Catalog 2013

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