Zero-dispersion wavelength
The wavelength at which a fiber's chromatic dispersion crosses zero, near 1310 nm in standard single-mode fiber. Pulse spreading is minimal there. Unfortunately, four-wave mixing is maximal there too.
Chromatic dispersion in fiber is the sum of two contributions with opposite trends: material dispersion (silica's index curvature, negative below ~1270 nm and positive above) and waveguide dispersion (geometry-dependent, negative in conventional designs). They cancel at the zero-dispersion wavelength .
For standard G.652 fiber, falls between roughly 1300 and 1324 nm. That is the historical reason the O-band was first home to telecom, and the ongoing reason datacom's 1310 nm intensity-modulated links (where no EDFA is available anyway) enjoy essentially free dispersion. Around , dispersion grows linearly with the slope ps/(nm²·km); by 1550 nm, standard fiber has climbed to ps/(nm·km).
Because waveguide dispersion is a design knob, can be relocated. Dispersion-shifted fiber (G.653) dragged it to 1550 nm to align zero dispersion with lowest loss. It promptly taught the industry a lesson: zero is the worst possible dispersion for WDM. Four-wave mixing between channels is phase-matched precisely where dispersion vanishes; DWDM channels riding near intermodulate catastrophically. The correction, non-zero dispersion-shifted fiber (G.655), parks a small but deliberately nonzero dispersion (~4–8 ps/nm/km) in the C-band: enough walk-off to spoil FWM phase matching, little enough to ease compensation. Coherent-era systems, able to digitally absorb any dispersion, closed the argument in the opposite direction: plain G.652 with its large 1550 nm dispersion is now the preferred long-haul medium, nonlinearity-suppressing and cheap.
Two practical notes. Fiber datasheets specify and per fiber design. Dispersion at any wavelength follows from the standard interpolation formula, which is how link totals get computed. And in nonlinear work the sign convention flips vocabulary: operation just above (anomalous dispersion) is where solitons and most Kerr-comb states live, making 's location a design input for nonlinear devices, not just links.