Page 1 Lecture 17 The applications of tomography: LTAO, MCAO, MOAO, GLAO Claire Max AY 289 UC Santa...

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Page 1 Lecture 17 Lecture 17 The applications of tomography: The applications of tomography: LTAO, MCAO, MOAO, GLAO LTAO, MCAO, MOAO, GLAO Claire Max AY 289 UC Santa Cruz March 7, 2013

Transcript of Page 1 Lecture 17 The applications of tomography: LTAO, MCAO, MOAO, GLAO Claire Max AY 289 UC Santa...

Page 1: Page 1 Lecture 17 The applications of tomography: LTAO, MCAO, MOAO, GLAO Claire Max AY 289 UC Santa Cruz March 7, 2013.

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Lecture 17Lecture 17

The applications of The applications of

tomography:tomography:

LTAO, MCAO, MOAO, GLAOLTAO, MCAO, MOAO, GLAO

Claire MaxAY 289

UC Santa CruzMarch 7, 2013

Page 2: Page 1 Lecture 17 The applications of tomography: LTAO, MCAO, MOAO, GLAO Claire Max AY 289 UC Santa Cruz March 7, 2013.

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Outline of lectureOutline of lecture

• What is AO tomography?

• AO applications of tomography

– Laser tomography AO

– Multi-conjugate AO (MCAO)

– Multi-object AO (MOAO)

– Ground-layer AO (GLAO)

• Much of this lecture is based on presentations by Don

Gavel, Lisa Poyneer, and Olivier Guyon. Thanks!

Page 3: Page 1 Lecture 17 The applications of tomography: LTAO, MCAO, MOAO, GLAO Claire Max AY 289 UC Santa Cruz March 7, 2013.

3

Limitations for AO systems with one guide star

• Isoplanatic AngleLimits the corrected field

θ0h

r0

Page 4: Page 1 Lecture 17 The applications of tomography: LTAO, MCAO, MOAO, GLAO Claire Max AY 289 UC Santa Cruz March 7, 2013.

4

Limitations for AO systems with one guide star

• Cone effect

Page 5: Page 1 Lecture 17 The applications of tomography: LTAO, MCAO, MOAO, GLAO Claire Max AY 289 UC Santa Cruz March 7, 2013.

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Limitations for AO systems with one guide star

• Cone effect1. Missing turbulence

outside and above cone

2. Spherical wave “stretching” of wavefront

More severe for larger telescope diameters

h

r0

Page 6: Page 1 Lecture 17 The applications of tomography: LTAO, MCAO, MOAO, GLAO Claire Max AY 289 UC Santa Cruz March 7, 2013.

Fundamental problem to solve: Isoplanatic Angle

If we assume perfect on-axis correction,

and a single turbulent layer at altitude h,

the variance (sq. radian) is :

σ2

= 1.03 (θ/θ0)5/3

Where α is the angle to the optical axis,

θ0 is the isoplanatic angle:

θ0 = 0.31 (r0/h)

D = 8 m, r0 = 0.8 m,

h = 5 km θ0 = 10”

h

Page 7: Page 1 Lecture 17 The applications of tomography: LTAO, MCAO, MOAO, GLAO Claire Max AY 289 UC Santa Cruz March 7, 2013.

Fundamental problem to solve: Isoplanatic Angle

If we assume perfect on-axis correction, and a single turbulent layer at altitude h, the variance (sq. radian) is :σ2 = 1.03 (θ/θ0)

5/3

Where α is the angle to the optical axis, θ0 is the isoplanatic angle:θ0

= 0.31 (r0/h)

D = 8 m, r0 = 0.8 m, h = 5 km θ0

= 10”

h

Page 8: Page 1 Lecture 17 The applications of tomography: LTAO, MCAO, MOAO, GLAO Claire Max AY 289 UC Santa Cruz March 7, 2013.

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Francois RigautFrancois Rigaut’’s diagrams of s diagrams of tomography for AOtomography for AO

90 k

m

“Missing” Data

Credit: Rigaut, MCAO for Dummies

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What is Tomography ?What is Tomography ?2. Wider field of view, no cone effect2. Wider field of view, no cone effect

90 k

m

Credit: Rigaut, MCAO for Dummies

Tomography lets you reconstruct turbulence in the entire cylinder of air above the telescope mirror

Page 10: Page 1 Lecture 17 The applications of tomography: LTAO, MCAO, MOAO, GLAO Claire Max AY 289 UC Santa Cruz March 7, 2013.

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Concept of a metapupilConcept of a metapupil

• Can be made larger than “real” telescope pupil

• Increased field of view due to overlap of fields toward multiple guide stars

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11

• Each wavefront sensor measures the integral of index variation along the ray lines

• The line integral along z determines the kz=0 Fourier spatial frequency

component

• Projections at several angles sample the kx,ky,kz volume

kX

kZ

Fourier slice theorem in tomography(Kak, Computer Aided Tomography, 1988)

How tomography works: from Don How tomography works: from Don GavelGavel

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12

kX

kZ

• The larger the telescope’s primary mirror, the wider the range of angles accessible for measurement

• In Fourier space, this means that the “bow-tie” becomes wider

• More information about the full volume of turbulence above the telescope

How tomography works: from Don How tomography works: from Don GavelGavel

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y

How tomography works: some How tomography works: some mathmath

• Assume we measure y with our wavefront sensors

• Want to solve for x = value of δOPD)

• The equations are underdetermined – there are more unknown voxel values than measured phases ⇒ blind modes. Need a few natural guide stars to determine these.

• wherey = vector of all WFS measurementsx = value of δOPD) at each voxel in turbulent volume above telescope

x

A is a forward propagator

Page 14: Page 1 Lecture 17 The applications of tomography: LTAO, MCAO, MOAO, GLAO Claire Max AY 289 UC Santa Cruz March 7, 2013.

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y

x

Solve for the full turbulence above Solve for the full turbulence above the telescope using the back-the telescope using the back-propagatorpropagator

y

x

AT is a back propagator along rays back toward the guidestars

y = vector of all WFS measurements

x = value of δOPD) at each voxel in turbulent volume above telescope

Use iterative algorithms to converge on the solution.

Page 15: Page 1 Lecture 17 The applications of tomography: LTAO, MCAO, MOAO, GLAO Claire Max AY 289 UC Santa Cruz March 7, 2013.

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Tomography movie: RagazzoniTomography movie: Ragazzoni

Page 16: Page 1 Lecture 17 The applications of tomography: LTAO, MCAO, MOAO, GLAO Claire Max AY 289 UC Santa Cruz March 7, 2013.

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LGS Related Problems: LGS Related Problems: ““Null Null modesmodes””

• Five “Null Modes” are not seen by LGS (Tilt indetermination problem)→ Need 3 well spread

NGSs to control these modes

• Tilt Anisoplanatism : Low order modes (e.g. focus) > Tip-Tilt at altitude

→ Dynamic Plate Scale changes

Credit: Rigaut, MCAO for Dummies

Page 17: Page 1 Lecture 17 The applications of tomography: LTAO, MCAO, MOAO, GLAO Claire Max AY 289 UC Santa Cruz March 7, 2013.

Page 17

Outline of lectureOutline of lecture

• Review of AO tomography concepts

• AO applications of tomography

– Laser tomography AO

– Multi-conjugate AO (MCAO)

– Multi-object AO (MOAO)

– Ground-layer AO (GLAO)

Page 18: Page 1 Lecture 17 The applications of tomography: LTAO, MCAO, MOAO, GLAO Claire Max AY 289 UC Santa Cruz March 7, 2013.

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The multi-laser guide star AO zoo The multi-laser guide star AO zoo (1)(1)

Narrow field, suffers from cone effect

Narrow field, cone effect fixed

Page 19: Page 1 Lecture 17 The applications of tomography: LTAO, MCAO, MOAO, GLAO Claire Max AY 289 UC Santa Cruz March 7, 2013.

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The multi-laser guide star AO zoo The multi-laser guide star AO zoo (2)(2)

Both correct over a wide field, at a penalty in peak Strehl

Page 20: Page 1 Lecture 17 The applications of tomography: LTAO, MCAO, MOAO, GLAO Claire Max AY 289 UC Santa Cruz March 7, 2013.

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The multi-laser guide star AO zoo The multi-laser guide star AO zoo (3)(3)

Correct over narrow field of view located anywhere w/in

wide field of regard

Quite modest correction over a very wide field of

view

Page 21: Page 1 Lecture 17 The applications of tomography: LTAO, MCAO, MOAO, GLAO Claire Max AY 289 UC Santa Cruz March 7, 2013.

Central parts of the globular cluster Omega Centauri, as seen using different adaptive optics techniques. The upper image is a reproduction of ESO Press Photo eso0719, with the guide stars used for the MCAO correction identified with a cross. A box shows a 14 arcsec area that is then observed while applying different or no AO corrections, as shown in the bottom images. From left to right : No Adaptive Optics, Single Conjugate and Multi-Conjugate Adaptive Optics corrections. SCAO has almost no effect in sharpening the star images while the improvement provided by MCAO is remarkable.

Credit: ESO

MCAO on-sky performanceMCAO improves image quality where there is no single nearby bright guide star

Page 22: Page 1 Lecture 17 The applications of tomography: LTAO, MCAO, MOAO, GLAO Claire Max AY 289 UC Santa Cruz March 7, 2013.

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Outline of lectureOutline of lecture

• Review of AO tomography concepts

• AO applications of tomography– Multi-conjugate adaptive optics (MCAO)– Multi-object adaptive optics (MOAO)– Ground-layer AO (GLAO)

Page 23: Page 1 Lecture 17 The applications of tomography: LTAO, MCAO, MOAO, GLAO Claire Max AY 289 UC Santa Cruz March 7, 2013.

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What is multiconjugate AO?What is multiconjugate AO?

Deformable mirror

Turbulence Layers

Credit: Rigaut, MCAO for Dummies

Page 24: Page 1 Lecture 17 The applications of tomography: LTAO, MCAO, MOAO, GLAO Claire Max AY 289 UC Santa Cruz March 7, 2013.

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Deformable mirrors Turbulence Layers

Credit: Rigaut, MCAO for Dummies

What is multiconjugate AO?What is multiconjugate AO?

Page 25: Page 1 Lecture 17 The applications of tomography: LTAO, MCAO, MOAO, GLAO Claire Max AY 289 UC Santa Cruz March 7, 2013.

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The multi-conjugate AO conceptThe multi-conjugate AO concept

Telescope

DM1 DM2

Turb. Layers#2 #1

Atmosphere

WFS

UP

Credit: Rigaut, MCAO for Dummies

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Difference between Laser Difference between Laser Tomography AO and MCAOTomography AO and MCAO

• Laser Tomography AO can be done with only 1 deformable mirror

• If used with multiple laser guide stars, reduces cone effect

• MCAO uses multiple DMs, increases field of view

Page 27: Page 1 Lecture 17 The applications of tomography: LTAO, MCAO, MOAO, GLAO Claire Max AY 289 UC Santa Cruz March 7, 2013.

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WFSs

Guide Stars

DM2

Telescope

High Altitude Layer

Ground Layer

DM1WFC

““Star Oriented” MCAOStar Oriented” MCAO

• Each WFS looks at one star

• Global Reconstruction

• n GS, n WFS, m DMs

• 1 Real Time Controller

• The correction applied at each DM is computed using all the input data.

Credit: N. Devaney

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WFC2

DM2

WFS2

WFC1

DM1

WFS1

Telescope

High Alt. Layer

Ground Layer

Guide Stars

Layer Oriented MCAOLayer Oriented MCAO

• Layer Oriented WFS architecture

• Local Reconstruction

• x GS, n WFS, n DMs

• n RTCs

• Wavefront is reconstructed at each altitude independently.

• Each WFS is optically coupled to all the others.

• GS light co-added for better SNR.

Credit: N. Devaney

Page 29: Page 1 Lecture 17 The applications of tomography: LTAO, MCAO, MOAO, GLAO Claire Max AY 289 UC Santa Cruz March 7, 2013.

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MCAO Simulations, 3 laser guide MCAO Simulations, 3 laser guide starsstars

Strehl at 2.2 μm3 NGS, FoV = 1.5 arc min

Strehl at 2.2 μm3 NGS, FoV = 1 arc min

Credit: N. Devaney

As field of view increases, average Strehl drops and variation over

field increases

As field of view increases, average Strehl drops and variation over

field increases

Page 30: Page 1 Lecture 17 The applications of tomography: LTAO, MCAO, MOAO, GLAO Claire Max AY 289 UC Santa Cruz March 7, 2013.

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VLT Multi-conjugate AO VLT Multi-conjugate AO Demonstrator (MAD) showed that Demonstrator (MAD) showed that MCAO worksMCAO works

• Originally built as a technical demo to exercise in the lab, and then on the sky

• Compare layer-oriented with star-oriented MCAO

• Uses natural guide stars Users love it! Became

a regular VLT instrument

Page 31: Page 1 Lecture 17 The applications of tomography: LTAO, MCAO, MOAO, GLAO Claire Max AY 289 UC Santa Cruz March 7, 2013.

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Results from ESOResults from ESO’’s Multiconjugate s Multiconjugate AO Demonstrator (MAD)AO Demonstrator (MAD)

Single Conjugate Multi Conjugate

Effective θ0 ~ 20” Effective θ0 ~ 40-50”

Page 32: Page 1 Lecture 17 The applications of tomography: LTAO, MCAO, MOAO, GLAO Claire Max AY 289 UC Santa Cruz March 7, 2013.

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Science papers with MAD: Orion Science papers with MAD: Orion star clusterstar cluster

• MCAO correction is clearly better than single conjugate AO, but this is the case all across the image (not clear what θ0 is doing)

Page 33: Page 1 Lecture 17 The applications of tomography: LTAO, MCAO, MOAO, GLAO Claire Max AY 289 UC Santa Cruz March 7, 2013.

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Orion star cluster with MAD, Orion star cluster with MAD, continuedcontinued

Page 34: Page 1 Lecture 17 The applications of tomography: LTAO, MCAO, MOAO, GLAO Claire Max AY 289 UC Santa Cruz March 7, 2013.

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Jupiter with MAD: single conjugate Jupiter with MAD: single conjugate AO has done as well or better AO has done as well or better than MCAOthan MCAO

MAD MCAO Regular Keck AO

Jupiter is about 30” across

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Early impressions of MCAO Early impressions of MCAO performance based on MAD performance based on MAD results to dateresults to date

• Can extend θ0 from ~ 20 arc sec all the way to ~ 60”

• Some penalty in peak Strehl, in return for larger corrected field

• But really need three guide stars - hard to find if using “real” stars. (Hence MAD’s lopsided Strehl maps.)

• MCAO should really excel with laser guide stars– Gemini South’s GEMS is first to do this

• Note: Solar AO has demonstrated benefits of MCAO using multiple “regions of interest” as wavefront references

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GEMS image of star formation in GEMS image of star formation in OrionOrion

Page 39: Page 1 Lecture 17 The applications of tomography: LTAO, MCAO, MOAO, GLAO Claire Max AY 289 UC Santa Cruz March 7, 2013.

• Orion star forming region:

• Compare GEMS MCAO with ALTAIR single conjugate AO on Gemini North Telescope

ALTAIR GEMS

Page 40: Page 1 Lecture 17 The applications of tomography: LTAO, MCAO, MOAO, GLAO Claire Max AY 289 UC Santa Cruz March 7, 2013.

Page 40

Outline of lectureOutline of lecture

• Review of AO tomography concepts

• AO applications of tomography– Multi-conjugate adaptive optics (MCAO)– Multi-object adaptive optics (MOAO)– Ground-layer AO (GLAO)

Page 41: Page 1 Lecture 17 The applications of tomography: LTAO, MCAO, MOAO, GLAO Claire Max AY 289 UC Santa Cruz March 7, 2013.

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Distinctions between multi-Distinctions between multi-conjugate and multi-object AOconjugate and multi-object AO

• DMs conjugate to different altitudes in the atmosphere

• Guide star light is corrected by DMs before its wavefront is measured

• Only one DM per object, conjugate to ground

• Guide star light doesn’t bounce off small MEMS DMs in multi-object spectrograph

?

1-2 arc min

Page 42: Page 1 Lecture 17 The applications of tomography: LTAO, MCAO, MOAO, GLAO Claire Max AY 289 UC Santa Cruz March 7, 2013.

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Multi-Object AOMulti-Object AO

• Correct over multiple narrow fields of view located anywhere w/in wide field of regard

• In most versions, each spectrograph or imager has its own MEMS AO mirror, which laser guide star lights doesn’t bounce off of

• Hence this scheme is called “open loop”: DM doesn’t correct laser guide star wavefronts before LGS light goes to wavefront sensors

• In one version, each LGS also has its own MEMS correction

Page 43: Page 1 Lecture 17 The applications of tomography: LTAO, MCAO, MOAO, GLAO Claire Max AY 289 UC Santa Cruz March 7, 2013.

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Science with MOAO: multiple Science with MOAO: multiple deployable spatially resolved deployable spatially resolved spectrographsspectrographs

• A MEMS DM underneath each high-redshift galaxy, feeding a narrow-field spatially resolved spectrograph (IFU)

• No need to do AO correction on the blank spaces between the galaxies

Page 44: Page 1 Lecture 17 The applications of tomography: LTAO, MCAO, MOAO, GLAO Claire Max AY 289 UC Santa Cruz March 7, 2013.

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Why does MOAO work if there is Why does MOAO work if there is only one deformable mirror in the only one deformable mirror in the science path?science path?

• Tomography lets you measure the turbulence throughout the volume above the telescope

90 k

m

Page 45: Page 1 Lecture 17 The applications of tomography: LTAO, MCAO, MOAO, GLAO Claire Max AY 289 UC Santa Cruz March 7, 2013.

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Why does MOAO work if there is Why does MOAO work if there is only one deformable mirror in the only one deformable mirror in the science path?science path?

• Tomography lets you measure the turbulence throughout the volume above the telescope

• In the direction to each galaxy, you can then project out the turbulence you need to cancel out for that galaxy

90 k

m

Page 46: Page 1 Lecture 17 The applications of tomography: LTAO, MCAO, MOAO, GLAO Claire Max AY 289 UC Santa Cruz March 7, 2013.

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Existing and Near-Term MOAO Existing and Near-Term MOAO SystemsSystems

• CANARY (Durham, Obs. de Paris, ONERA, ESO)– MOAO demonstrator for E-ELT– On William Herschel Telescope; one arm– Had already commissioning run – First NGS (done), then Rayleigh guide stars

• RAVEN (U Victoria, Subaru, INO, Canadian NRC)– And Celia Blain!– MOAO demonstrator for Subaru telescope– 3 NGS wavefront sensors– Field of regard > 2.7 arc min– Will feed an IR science camera – Delivery in 2012

Page 47: Page 1 Lecture 17 The applications of tomography: LTAO, MCAO, MOAO, GLAO Claire Max AY 289 UC Santa Cruz March 7, 2013.
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VILLAGES at Lick Observatory: VILLAGES at Lick Observatory: Demonstration of Open-Loop Demonstration of Open-Loop PerformancePerformance

• Initial demonstration of open-loop MEMS performance– VILLAGES experiment on 1-meter telescope at

Mount Hamilton (Lick Observatory)– It works!

Page 49: Page 1 Lecture 17 The applications of tomography: LTAO, MCAO, MOAO, GLAO Claire Max AY 289 UC Santa Cruz March 7, 2013.

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Both E-ELT and TMT have done Both E-ELT and TMT have done early designs for MOAO systemsearly designs for MOAO systems

• Artist’s sketch of EAGLE MOAO system for E-ELT

• One of the constraints is that the spectrographs are very large!

• Hard (and expensive) to fit in a lot of them

Page 51: Page 1 Lecture 17 The applications of tomography: LTAO, MCAO, MOAO, GLAO Claire Max AY 289 UC Santa Cruz March 7, 2013.

Page 51

Outline of lectureOutline of lecture

• Review of AO tomography concepts

• AO applications of tomography– Multi-conjugate adaptive optics (MCAO)– Multi-object adaptive optics (MOAO)– Ground-layer AO (GLAO)

Page 52: Page 1 Lecture 17 The applications of tomography: LTAO, MCAO, MOAO, GLAO Claire Max AY 289 UC Santa Cruz March 7, 2013.

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Ground layer AO: do tomography, Ground layer AO: do tomography, but only use 1 DM (conjugate to but only use 1 DM (conjugate to ground layer)ground layer)

single DM conjugated to ground layer

Credit: J-M Conan

GLAO uses 1 ground-conjugated DM, corrects near-ground turbulence

MCAO GLA

O

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Correcting just the ground layer Correcting just the ground layer gives a very large isoplanatic gives a very large isoplanatic angleangle

• Strehl = 0.38 at θ = θ0

θ0 is isoplanatic angle

θ0 is weighted by high-altitude turbulence (z5/3)

• If turbulence is only at low altitude, overlap is very high.

• If you only correct the low altitude turbulence, the isoplanatic angle will be large (but the correction will be only modest) Telescope

Common Path

Page 54: Page 1 Lecture 17 The applications of tomography: LTAO, MCAO, MOAO, GLAO Claire Max AY 289 UC Santa Cruz March 7, 2013.

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Ground Layer AO (GLAO) typically Ground Layer AO (GLAO) typically decreases natural decreases natural ““seeingseeing”” by a by a factor of 1.5 to 2factor of 1.5 to 2

• Example: GLAO calculation for Giant Magellan Telescope (M. Johns)

• Adaptive secondary conjugation at 160 m above primary mirror.

• Performance goals:

– λ > 0.8 μm

– Field of view: >10’

– Factor of 1.5-2 reduction in image size. Modeled using Cerro Pachon

turbulence profile. (M-L Hart 2003)

Page 55: Page 1 Lecture 17 The applications of tomography: LTAO, MCAO, MOAO, GLAO Claire Max AY 289 UC Santa Cruz March 7, 2013.

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Many observatories have Many observatories have ambitious GLAO projects plannedambitious GLAO projects planned

• Near term on medium sized telescopes: SOAR (4.25m), William Herschel Telescope (4.2m), MMT (6.5m)

• Medium term on VLT (8m), LBT (2x8m)

• Longer term on Giant Magellan Telescope etc.

• Is it worth the large investment “just” to decrease “seeing” disk by factor of 1.5 to 2 ?

– Depends on whether existing or planned large spectrographs can take advantage of smaller image

– Potential improved SNR for background-limited point sources

Page 56: Page 1 Lecture 17 The applications of tomography: LTAO, MCAO, MOAO, GLAO Claire Max AY 289 UC Santa Cruz March 7, 2013.

Page 56 Credit: A.

Tokovinin

time

Page 57: Page 1 Lecture 17 The applications of tomography: LTAO, MCAO, MOAO, GLAO Claire Max AY 289 UC Santa Cruz March 7, 2013.

Page 57 Credit: A.

Tokovinin

Page 58: Page 1 Lecture 17 The applications of tomography: LTAO, MCAO, MOAO, GLAO Claire Max AY 289 UC Santa Cruz March 7, 2013.

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Initial demonstration of GLAO at Initial demonstration of GLAO at MMTMMT

• With GLAO, image width is reduced from 0.70 to 0.33 arc sec and peak intensity is increased by factor of 2.3

• Credit: Christoph Baranec, Michael Hart, and colleagues, U AZ

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Page 60: Page 1 Lecture 17 The applications of tomography: LTAO, MCAO, MOAO, GLAO Claire Max AY 289 UC Santa Cruz March 7, 2013.

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GLAO at the MMT (Rayleigh guide GLAO at the MMT (Rayleigh guide stars)stars)

Page 61: Page 1 Lecture 17 The applications of tomography: LTAO, MCAO, MOAO, GLAO Claire Max AY 289 UC Santa Cruz March 7, 2013.

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SOAR Telescope

Page 62: Page 1 Lecture 17 The applications of tomography: LTAO, MCAO, MOAO, GLAO Claire Max AY 289 UC Santa Cruz March 7, 2013.

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SummarySummary

• Tomography: a way to measure the full volume of turbulence above the telescope

• Once you have measured the turbulence there are several ways to do the wavefront correction

– Laser Tomography AO: Multiple laser guide stars, 1 DM, corrects cone effect. Narrow field.

– Multi-conjugate AO: Multiple DMs, each optically conjugate to a different layer in atmosphere. Wider field of view.

– Multi-object AO: Correct many individual objects, each over a small field. Each has very good correction. Wider field of regard.

– Ground-layer AO: Correct just ground layer turbulence. Very large field of view but only modest correction.

• All four methods will be used in the future

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Backup slidesBackup slides

Page 64: Page 1 Lecture 17 The applications of tomography: LTAO, MCAO, MOAO, GLAO Claire Max AY 289 UC Santa Cruz March 7, 2013.

Alt

itu

de

Cn2

n

(Turbulence Strength) (Index variations)Projection

Cn2

weighted back-

projection

Uniformly weighted back-

projection

5-guidestar

reconstructions

Reconstruction using back-projections with CReconstruction using back-projections with CNN22

x

GS1 GS2S

z

Page 65: Page 1 Lecture 17 The applications of tomography: LTAO, MCAO, MOAO, GLAO Claire Max AY 289 UC Santa Cruz March 7, 2013.

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Cone (laser guide star) back-projectionsCone (laser guide star) back-projections

Alt

itu

de

n

(Index variations)

3 laser guidestar reconstuction 5 laser guidestar

reconstuction

5 natural star reconstuction

x

GS1 GS2S

z