Laser basics Optics, Eugene Hecht, Chpt. 13; Optical resonator tutorial:
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Transcript of Laser basics Optics, Eugene Hecht, Chpt. 13; Optical resonator tutorial:
![Page 1: Laser basics Optics, Eugene Hecht, Chpt. 13; Optical resonator tutorial:](https://reader033.fdocuments.net/reader033/viewer/2022061614/56649dce5503460f94ac1ff0/html5/thumbnails/1.jpg)
Laser basics
Optics, Eugene Hecht, Chpt. 13;
Optical resonator tutorial: http://www.dewtronics.com/tutorials/lasers/leot/
![Page 2: Laser basics Optics, Eugene Hecht, Chpt. 13; Optical resonator tutorial:](https://reader033.fdocuments.net/reader033/viewer/2022061614/56649dce5503460f94ac1ff0/html5/thumbnails/2.jpg)
Laser oscillationLaser is oscillator
• Like servo with positive feedback
• Greater than unity gain
Ruby laser example
Laser turn-on and gain saturation
Laser gain and losses
Gain decreases as output power increases• Saturation
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Fabry-Perot cavity for feedback• High reflectivity mirrors
• Low loss per round trip
• Must remember resonance conditions– round trip path is multiple of
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• High reflectivity Fabry-Perot cavity• Boundary conditions
– field is zero on mirrors• Multiple wavelengths possible
– agrees with resonance conditions
Laser longitudinal modesClassical mechanics analog
Multi-mode laser
Fabry-Perot boundary conditions
Multiple resonant frequencies
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Single longitudinal mode lasers• Insert etalon into cavity
• Use low reflectivity etalon– low loss
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Laser transverse modes• Wave equation looks like harmonic oscillator
• Ex: E = E e -it
• Separate out z dependence
• Solutions for x and y are Hermite polynomials
Frequencies of transverse modes
Transverse laser modes
02
2
Ec
nE
02
2
xm
k
dt
xd
02 22
2
2
2
2
2
2
Ekc
n
y
E
x
E
z
Eik
z
E
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Single transverse mode lasers• Put aperture in laser
• Create loss for higher order modes
Multi-longitudinal Multi-transverse&long. Single mode
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Gaussian beams• Zero order mode is Gaussian
• Intensity profile:
• beam waist: w0
• confocal parameter: z
• far from waist
• divergence angle
22 /20
wreII
2
20
0 1
w
zww
2
0wzR
0w
zw
00
637.02
ww
Gaussian propagation
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Power distribution in Gaussian• Intensity distribution:• Experimentally to measure full width at half maximum (FWHM) diameter
• Relation is dFWHM = w 2 ln2 ~ 1.4 w
• Define average intensity
• Iavg = 4 P / ( d2FWHM)
• Overestimates peak: I0 = Iavg/1.4
22 /20
wreII
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Resonator options• Best known -- planar, concentric, confocal• Confocal unique
– mirror alignment not critical– position is critical– transverse mode frequencies identical
Types of resonators
Special cases