Phase velocity
velocity with which phase fronts propagated in a medium: v_ph
more general term: velocity of light
considered for: plane waves, where wavefronts are simply moving in a direction perpendicular to their orientation
related to wavenumber k and (angular) optical frequency ω:
in vacuum: phase velocity equals speed of light, c = 299,792,458 m/s, independent of optical frequency + equal to group velocity
in medium: phase velocity smaller than c, by refractive index n.
In visible spectral region: typical transparent crystals & optical glasses have n between 1.4 & 2.8, semicond. higher
in X-ray region: refractive indices are slightly below 1
-> corresponds to phase velocity slightly above vacuum velocity of light
-> similar effects caused e.g. by optical resonances of atoms in visible spectral region
-> this does not allow for superluminal transmission of information, or for violating causality
Photonic metamaterials
can create: negative-index media
this can cause: phase velocity can be directed in opposite to the direction of the energy flow
wavefronts of focused lased beam
due to Gouy phase shift, these move slightly faster near the focus
wavenumber
phase delay per unit length, or that quantity devided by 2π:
-> λ is the wavelength in the medium (not the vacuum wavelength)
angular wavenumber: magnitude of wave vector
= phase delay per unit length during propagation of plane wave
in spectroscopy, wavenumber is:
-> usually considered in vacuum
Light in a medium: wavenumber = vacuum wavenumber * refractive index
wavenumber related to phase change per unit length of a plane wave in homogeneous medium
-> for focused beams: phase change per unit length is modified with respect to that for a plane wave
-> for Gaussian beams: this modification is Gouy phase shift
-> for propagation of guided waves in waveguides: imaginary part of propagation constant γ (called β) is the relevant quantity
optical frequency
= oscillation freq. of the corresponding electromagnetic wave
calculated with: ν = c / λ
visible light: 400 THz - 700 THz = 700 nm to 400 nm
angular freq: ω = 2π ν
optical power usually distributed over some freq. range, sometimes spends a whole octave (i.e. a factor of two in terms of freq.) or even substantially more
highly freq.-stabilized lasers:
-> can produce light with very small optical bandwidth, sometimes even below 1 Hz (= extremely small fraction of mean optical freq. of 100s of THz + very high stability of that freq.)
-> also called “optical freq. standards“; required for optical clocks
opt. freq. can be measured far more precisely than wavelengths: “freq. metrology“
-> not directly detected like
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