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Final state effects in quantum fluids

Conference ·
The extraction of momentum distributions from high energy scattering experiment depends on the validity of the impulse approximation (IA) which has been extensively discussed in the workshop overview. The IA assumes that in the scattering process the kinetic energy imparted to a recoiling particle is large compared to the potential energy due to neighboring particles. While this may be true for x-ray Compton scattering from electronic systems, it is less true for quasielastic electron-nucleus scattering, and it is invalid for deep inelastic neutron scattering (DINS) from quantum fluids and solids such as helium. In the latter case, the interatomic potential has a steeply repulsive core which is never negligible compared to the kinetic energies which can be imparted in feasible neutron scattering experiments. The corrections to the IA due to interactions of the recoiling atom with neighboring atoms are termed ''final state effects'' (FSE). This paper presents the theory of FSE for the case of deep inelastic neutron scattering from /sup 4/He quantum fluids. The lessons should also be applicable to momentum distribution experiments in many other systems. 28 refs., 12 figs.
Research Organization:
Los Alamos National Lab., NM (USA)
DOE Contract Number:
W-7405-ENG-36
OSTI ID:
6398822
Report Number(s):
LA-UR-89-205; CONF-8810118-3; ON: DE89006525
Country of Publication:
United States
Language:
English