Photonica

Phase velocity

The speed at which the crests of a single-frequency wave move, v_p = c/n = ω/k. In a dispersive medium it differs from the group velocity at which pulses and information travel: in fused silica at 1550 nm about 207,600 km/s against 205,000 km/s.

Optics fundamentalsUpdated September 2026

A monochromatic wave cos⁡(kz−ωt)\cos(kz - \omega t) has crests that advance at the phase velocity

vp=ωk=cn,v_p = \frac{\omega}{k} = \frac{c}{n},

where nn is the refractive index or, for a guided mode, the effective index, and kk is the propagation constant. It is the velocity that sets wavelength in the medium, phase matching in nonlinear optics, and the phase accumulated in an interferometer arm.

A pulse or any modulated signal is a superposition of frequencies, and its envelope moves at the group velocity, vg=dω/dk=c/ngv_g = d\omega/dk = c/n_g, with the group index ng=n−λ dn/dλn_g = n - \lambda\,dn/d\lambda. In normal dispersion, where the index falls with wavelength, ng>nn_g > n and the envelope is slower than the crests, which slide forward through it. In fused silica at 1550 nm, n≈1.444n \approx 1.444 gives a phase velocity of about 207,600 km/s, while the bulk group index of 1.463 gives about 205,000 km/s (in standard fiber the group index is 1.468 and the group velocity 204,200 km/s); in a silicon wire waveguide the difference is much larger, with effective index about 2.4 and group index above 4 in typical designs.

Faster than light

The phase velocity can exceed cc, and does whenever the index is below 1: for X-rays in matter, near an absorption line on its high-frequency side, and for any waveguide mode close to cutoff in a metallic waveguide. This carries no information, because a single frequency extending forever cannot signal. The speed of a signal front never exceeds cc, which Sommerfeld and Brillouin showed in 1914; group velocity can also exceed cc in anomalously dispersive media without signalling faster than light, because the pulse reshapes rather than travelling undistorted.

Measurement

Phase velocity follows from a measured index or effective index: from the angle of refraction, from a prism at minimum deviation, from ellipsometry for thin films, or for waveguides from the angle at which a grating coupler couples light in. Interferometers measure phase delay, nLn L, directly. The group index is measured separately, from a pulse delay or from the fringe spacing of a resonator.

References: M. Born, E. Wolf, Principles of Optics, 7th ed. (Cambridge University Press, 1999), Ch. 1; L. Brillouin, Wave Propagation and Group Velocity (Academic Press, 1960).