Inelastic scattering of light by matter, creating noise in optical fibers.Raman scattering is the inelastic scattering of photons by matter, where the scattered light gains or loses energy corresponding to vibrational or rotational transitions in the scattering molecules. Unlike Rayleigh scattering (elastic), Raman scattering shifts the photon's frequency, producing a spectrum that fingerprints the material's molecular structure. In optical fibers, it is a nuisance: it limits the power that can be transmitted by converting some light into unwanted wavelengths, but it also enables amplifiers and sensors.
The effect was predicted by Adolf Smekal in 1923 and experimentally confirmed by C.V. Raman and K.S. Krishnan in 1928, for which Raman received the Nobel Prize in Physics in 1930.
A photon interacts with a molecule, exciting it to a virtual energy state that is not a real quantum level. The molecule then relaxes to a different vibrational state, emitting a photon with energy equal to the incident photon minus (Stokes) or plus (anti-Stokes) the vibrational quantum. The intensity and frequency shifts of these scattered photons reveal the molecular bond energies and symmetries, making Raman spectroscopy a powerful analytical tool.
Raman scattering is used in fiber-optic communication as distributed temperature sensors (DTS) and in Raman amplifiers, while in laboratories it powers non-destructive chemical analysis, from pharmaceutical quality control to the detection of explosives.
Only about one in ten million photons undergoes Raman scattering, which is why the effect is weak and required intense laser sources to become practically useful.




