Gaussian Beam in a Symmetric Confocal Resonator.

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SUMMARY

The discussion focuses on the analysis of a symmetric confocal resonator with a mirror spacing of 16 cm and reflectances of 0.995, operating at a wavelength of 1 μm. Key calculations include the radii of curvature of the mirrors, determined to be -16 cm, and the waist of the Gaussian mode, calculated as 0.1596 mm. The resonance frequencies for the (0,0) and (1,0) modes are derived, yielding velocities of 4.913 x 10^8 m/s and 8.042 x 10^8 m/s, respectively. The distributed resonator loss coefficient Qr is computed to be 0.2351 x 10^11 s^-1, indicating the impact of mirror reflectance on resonator performance.

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Homework Statement


A symmetric confocal resonator with mirror spacing d =16 cm, mirror reflectances 0.995, and n = 1 is used in a laser operating at λ[o] = 1 μm.
(a) Find the radii of curvature of the mirrors.
(b) Find the waist of the (0,0) (Gaussian) mode.
(c) Sketch the intensity distribution of the (1,0) modes at one of the mirrors and determine the distance between its two peaks.
(d) Determine the resonance frequencies of the (0,0) and (1,0) modes.
(e) Assuming that losses arise only from imperfect mirror reflectances, determine the distributed resonator loss coefficient Qr.



Homework Equations







The Attempt at a Solution


a) symmetric confocal ==> R1=R2=-d=-16cm.

Zo = d/2=8cm
b) W0=√(λ*d/2*pi) = 0.1596 mm

d)v[q]=qv[F] + (Δζ/pi) v[F]
 
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v[F]=c/n = 3x10^8 /1 = 3x10^8 m/sΔζ(q,p) = (p+1/2)*pi - arctan(2*pi*(2*q+p+1)*z0/λo) for (0,0): Δζ (0,0)= pi-arctan(2*pi*z0/λo)= pi- arctan(16*pi/1x10^-6) = 3.1415 rad for (1,0): Δζ (1,0)= 3/2*pi - arctan(2*pi*3*z0/λo)= 4.7122 radv[q,p]=(1+1/2)*v[F] + (Δζ/pi)* v[F] ==> v (0,0)= 1.5*v[F] + (3.1415/pi)*v[F]=4.913x10^8 m/s and v (1,0)= 2.5*v[F] + (4.7123/pi)*v[F]= 8.042x10^8 m/s e) Qr = (π*v[F])/((1-R^2)*A) where A = 4*pi*W0^2 Qr = (π*v[F]) / ((1-0.995^2)*4*pi*(0.1596x10^-3)^2) Qr= 0.2351x10^11 s^-1
 

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