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U.S. Department of Energy
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QUANTUM THEORY OF THE ENERGY SPECTRUM OF SUPERFLUIDS

Thesis/Dissertation ·
OSTI ID:4162925
An explicit formula for the energy eigenvalues for the low states of a superfluid is developed in a free phonon'' approximation; this formula exhibits clearly the quasiparticle nature of the excited states. Initially, a certain basis of correlated wave functions is assumed and used to construct an orthonormal basis. In the representation of the latter basis, the Hamiltonian has a particularly simple form, which is then diagonalized by a Bogoliubov-type frainsformation. The method and results can be applied to a system of strongly interacting particles, such as real system of He-4, as well as to a model system of weakly interacting particles. The energy formula yields the results obtained by Feynman and by Bogoliubov as special cases. Next the free phonon'' results are taken as a zerothorder approximation and used to calculate the correction to the dispersion curve for elementary excitations in the approximation of the Brillouin-Wigner second-order energy formula. The computed elementary energy spectrum is compared with the dispersion curve constracted from the single inelastic scattering of neutrons by Henshaw and Woods, andd with the theoretical curve obtained from a variational calculation by Feynman and Cohen. Approximations involved in the present calculation are discussed, and a discrepancy between theoretical and experimental energy values for excitations with small momentum is studied. A method for examining the stability of elementary excitations corresponding to both experimental and theoretical dispersion curves is presented and applied to the curves mentioned above. Finally criteria are developed which indicate the accuracy of approximations to the 3particle distribution function generated by the ground state of a quantum fluid. One criterion is applied to the Kirkwood superposition form for a system of He-4 in order to study the errors involved in the approximation; a related criterion is used to investigate the accuracy of approximations occurring in the second-order perturbation calculation described above. (Dissertation Abstr.)
Research Organization:
Originating Research Org. not identified
NSA Number:
NSA-18-000944
OSTI ID:
4162925
Country of Publication:
Country unknown/Code not available
Language:
English