Abstract
We study the ground state energy of a gas of 1D bosons with density ρ, interacting through a general, repulsive 2-body potential with scattering length a, in the dilute limit ρ|a|≪1. The first terms in the expansion of the thermodynamic energy density are (π2ρ3/3)(1+2ρa), where the leading order is the 1D free Fermi gas. This result covers the Tonks–Girardeau limit of the Lieb–Liniger model as a special case, but given the possibility that a>0, it also applies to potentials that differ significantly from a delta function. We include extensions to spinless fermions and 1D anyonic symmetries, and discuss an application to confined 3D gases.
Originalsprog | Engelsk |
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Artikelnummer | 27 |
Tidsskrift | Communications in Mathematical Physics |
Vol/bind | 406 |
Udgave nummer | 2 |
Antal sider | 41 |
ISSN | 0010-3616 |
DOI | |
Status | Udgivet - 2025 |
Bibliografisk note
Publisher Copyright:© The Author(s), under exclusive licence to Springer-Verlag GmbH Germany, part of Springer Nature 2024.