Gaussian Beam in a Symmetric Confocal Resonator.

In summary, we are given a symmetric confocal resonator with a mirror spacing of 16 cm and mirror reflectances of 0.995, used in a laser operating at 1 μm. We are asked to find the radii of curvature of the mirrors, the waist of the (0,0) mode, the intensity distribution of the (1,0) modes, the resonance frequencies of the (0,0) and (1,0) modes, and the distributed resonator loss coefficient Qr assuming losses only from imperfect mirror reflectances. After calculations, we find that the radii of curvature of the mirrors are -16 cm, the waist of the (0,0) mode is 0.1596
  • #1
mogul28
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0
λ

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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  • #2
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
 

What is a Gaussian Beam?

A Gaussian beam is a type of laser beam with a characteristic intensity distribution that follows a Gaussian or bell-shaped curve. It is often used in laser physics and optics due to its unique properties.

What is a Symmetric Confocal Resonator?

A symmetric confocal resonator is a type of resonator used in laser systems that consists of two concave mirrors facing each other and sharing the same focal point. This design allows for the propagation of a Gaussian beam with minimal divergence.

How does a Gaussian Beam behave in a Symmetric Confocal Resonator?

In a symmetric confocal resonator, a Gaussian beam will oscillate back and forth between the two mirrors, with each round trip causing the beam to become more focused and intense. This results in a highly collimated and stable output beam.

What are the advantages of using a Gaussian Beam in a Symmetric Confocal Resonator?

The use of a Gaussian beam in a symmetric confocal resonator offers several advantages, including high beam quality, low divergence, and stable output power. It also allows for the efficient use of laser energy and can produce a well-defined focal spot.

What are some applications of Gaussian Beam in a Symmetric Confocal Resonator?

Gaussian beams in symmetric confocal resonators are commonly used in laser cutting, welding, and drilling applications due to their high beam quality and precision. They are also used in scientific research, such as in spectroscopy and microscopy experiments.

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