Abstract
The propagation of zero sound in a spin-polarized Fermi gas under harmonic confinement is studied as a function of the mean-field interactions with a second Fermi gas. A local-density treatment is compared with the numerical solution of the Vlasov–Landau equations for the propagation of density distortions in a trapped two-component Fermi gas at temperature T=0.2 T F . The response of the gas to the sudden creation of a sharp hole at its centre is also studied numerically.
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