Cross-phase modulation (XPM) is a nonlinear optical effect where one wavelength of light can affect the phase of another wavelength of light through the optical Kerr effect. When the optical power from a wavelength impacts the refractive index, the impact of the new refractive index on another wavelength is known as XPM.
Applications of XPM Cross-phase modulation can be used as a technique for adding information to a light stream by modifying the phase of a coherent optical beam with another beam through interactions in an appropriate nonlinear medium. This technique is applied to fiber-optic communications. If both beams have the same wavelength, then this type of cross-phase modulation is degenerate. XPM is among the most commonly used techniques for quantum nondemolition measurements. Other advantageous applications of XPM include:
Nonlinear optical Pulse Compression of ultrashort pulses Passive mode-locking Ultrafast optical switching Demultiplexing of OTDM channels Wavelength conversion of WDM channels Measurement of nonlinear optical properties of the media (non-linear index n2 (Kerr nonlinearity) and nonlinear response relaxation time)
Disadvantages of XPM
XPM in DWDM applications In dense wavelength-division multiplexing (DWDM) applications with intensity modulation and direct detection (IM-DD), the effect of XPM is a two step process: First the signal is phase modulated by the copropagating second signal. In a second step dispersion leads to a transformation of the phase modulation into a power variation. Additionally, the dispersion results in a walk-off between the channels and thereby reduces the effect of XPM.
XPM leads to interchannel crosstalk in WDM systems It can produce amplitude and timing jitter
See also Self-phase modulation — SPM Four wave mixing — FWM Stimulated Raman scattering — SRS Cross-polarized wave generation — XPW
References
External links Cross-phase modulation (RP Photonics, Encyclopedia of Laser Physics and Technology)