quasielastic scattering
In physics, quasielastic scattering designates a limiting case of inelastic scattering, characterized by energy transfers being small compared to the incident energy of the scattered particles.
It was applied to thermal neutron scattering by Leon van Hove{{cite journal | last1=Van Hove | first1=L. | last2=McVoy | first2=K.W. | title=Pair distribution functions and scattering phenomena | journal=Nuclear Physics | publisher=Elsevier BV | volume=33 | year=1962 | issn=0029-5582 | doi=10.1016/0029-5582(62)90539-4 | pages=468–476| url=https://cds.cern.ch/record/343802 }} and Pierre Gilles de Gennes{{cite journal | last=de Gennes | first=P.G. | title=Collective motions of hydrogen bonds | journal=Solid State Communications | publisher=Elsevier BV | volume=1 | issue=6 | year=1963 | issn=0038-1098 | doi=10.1016/0038-1098(63)90212-6 | pages=132–137}}
(quasielastic neutron scattering, QENS).
Finally, it is sometimes used for dynamic light scattering (also known by the more expressive term photon correlation spectroscopy).