The phase velocity of laser light

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SUMMARY

The phase velocity of laser light in a vacuum is exactly equal to the speed of light, denoted as c. In dispersive media, the phase velocity can exceed c, but this does not imply any violation of relativity. The phase velocity is mathematically defined as v = w/k(w), where w is the frequency and k(w) is the wavenumber. The group velocity, which describes the speed of the pulse envelope, is defined as V = v(w)/(1-(w/v)(dv/dw), and can become negative or exceed c near strong transitions in resonant media.

PREREQUISITES
  • Understanding of wave mechanics and electromagnetic theory
  • Familiarity with concepts of phase velocity and group velocity
  • Knowledge of dispersive media and their properties
  • Basic mathematical skills to interpret equations involving frequency and wavenumber
NEXT STEPS
  • Research the mathematical derivation of phase and group velocity equations
  • Study the properties of dispersive media and their impact on wave propagation
  • Explore the implications of negative group velocity in quantum optics
  • Investigate practical applications of laser light in resonant media
USEFUL FOR

Physicists, optical engineers, and students studying wave phenomena, particularly those interested in the behavior of laser light in various media.

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What are the limitations on the phase velocity of laser light? Is it true to say that the phase velocity of laser light is limited to <c?
 
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That's true in vacuum, where is exactly c. Phase velocity in a medium has no meaning, I think; I've seen some cases where phase velocity is greater than c.
 
The phase velocity is defined as v = w/k(w), where w is the frequency and k(w) is the wavenumber, similar to 1/wavelength. I've allowed the medium to be dispersive, so k = k(w). The 'group velocity' is dw/dk.

One way to picture this is that a pulsed carrier wave will have two relevant velocities- the phase velocity is the velocity of the carrier wave, while the pulse envelope moves as per the group velocity.

If a pulse moves through resonant media, strange things happen to the group velocity but not to the phase velocity- the phase velocity is simply v = c/(1+X'(w)/2), where X'(w) is the frequency-dependent real part of the susceptibility. The group velocity V =v(w)/(1-(w/v)(dv/dw)) and can become negative or exceed c0 near strong transitions.
 

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