Multicomponent Fermi systems at low densities

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Auteurs principaux: Pethick, C. J., Schwenk, A.
Format: Preprint
Publié: 2024
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author Pethick, C. J.
Schwenk, A.
author_facet Pethick, C. J.
Schwenk, A.
contents We calculate, to second order in the scattering length between two fermions, the Landau quasiparticle interaction for a low-density mixture of two fermion species with unequal densities at temperature zero. From the Landau parameters we evaluate the energy density and find agreement with the result of Kanno, Prog. Theor. Phys. 44, 813 (1970). The calculations are then extended to the case of two fermion components with different total densities, each with two spin components, a situation of interest in nuclear physics and astrophysics, where the species are neutrons and protons. An interesting finding is that, for low proton concentrations, $x \ll 1$, the leading term in the energy density, beyond the $x^{5/3}$ contribution from the kinetic energy and the $x^2$ one due to the two-body interaction in the mean-field approximation, varies as $x^{7/3} \ln x$. This is to be contrasted with the higher powers of $x$ implicit in many phenomenological energy-density functionals employed in nuclear physics, such as those of the Skyrme type.
format Preprint
id arxiv_https___arxiv_org_abs_2409_16199
institution arXiv
publishDate 2024
record_format arxiv
spellingShingle Multicomponent Fermi systems at low densities
Pethick, C. J.
Schwenk, A.
Nuclear Theory
High Energy Astrophysical Phenomena
Quantum Gases
We calculate, to second order in the scattering length between two fermions, the Landau quasiparticle interaction for a low-density mixture of two fermion species with unequal densities at temperature zero. From the Landau parameters we evaluate the energy density and find agreement with the result of Kanno, Prog. Theor. Phys. 44, 813 (1970). The calculations are then extended to the case of two fermion components with different total densities, each with two spin components, a situation of interest in nuclear physics and astrophysics, where the species are neutrons and protons. An interesting finding is that, for low proton concentrations, $x \ll 1$, the leading term in the energy density, beyond the $x^{5/3}$ contribution from the kinetic energy and the $x^2$ one due to the two-body interaction in the mean-field approximation, varies as $x^{7/3} \ln x$. This is to be contrasted with the higher powers of $x$ implicit in many phenomenological energy-density functionals employed in nuclear physics, such as those of the Skyrme type.
title Multicomponent Fermi systems at low densities
topic Nuclear Theory
High Energy Astrophysical Phenomena
Quantum Gases
url https://arxiv.org/abs/2409.16199