Non-Hermitian $p$-wave superfluid and effects of the inelastic three-body loss in a one-dimensional spin-polarized Fermi gas

Fuente: arXiv
Saved in:
Bibliographic Details
Main Authors: Tajima, Hiroyuki, Sekino, Yuta, Inotani, Daisuke, Dohi, Akira, Nagataki, Shigehiro, Hayata, Tomoya
Format: Preprint
Published: 2023
Subjects:
Online Access:
Tags: Add Tag
No Tags, Be the first to tag this record!
_version_ 1866915246544781312
author Tajima, Hiroyuki
Sekino, Yuta
Inotani, Daisuke
Dohi, Akira
Nagataki, Shigehiro
Hayata, Tomoya
author_facet Tajima, Hiroyuki
Sekino, Yuta
Inotani, Daisuke
Dohi, Akira
Nagataki, Shigehiro
Hayata, Tomoya
contents We theoretically investigate non-Hermitian $p$-wave Fermi superfluidity in one-dimensional spin-polarized Fermi gases which is relevant to recent ultracold atomic experiments. Considering an imaginary atom-dimer coupling responsible for the three-body recombination process in the Lindblad formalism, we discuss the stability of the superfluid state against the atomic loss effect. Within the two-channel non-Hermitian BCS-Leggett theory, the atomic loss is characterized by the product of the imaginary atom-dimer coupling and the $p$-wave effective range. Our results indicate that for a given imaginary atom-dimer coupling, a smaller magnitude of the effective ranges of $p$-wave interaction is crucial for reaching the non-Hermitian $p$-wave Fermi superfluid state.
format Preprint
id arxiv_https___arxiv_org_abs_2312_15724
institution arXiv
publishDate 2023
record_format arxiv
spellingShingle Non-Hermitian $p$-wave superfluid and effects of the inelastic three-body loss in a one-dimensional spin-polarized Fermi gas
Tajima, Hiroyuki
Sekino, Yuta
Inotani, Daisuke
Dohi, Akira
Nagataki, Shigehiro
Hayata, Tomoya
Quantum Gases
Strongly Correlated Electrons
Superconductivity
Nuclear Theory
Quantum Physics
We theoretically investigate non-Hermitian $p$-wave Fermi superfluidity in one-dimensional spin-polarized Fermi gases which is relevant to recent ultracold atomic experiments. Considering an imaginary atom-dimer coupling responsible for the three-body recombination process in the Lindblad formalism, we discuss the stability of the superfluid state against the atomic loss effect. Within the two-channel non-Hermitian BCS-Leggett theory, the atomic loss is characterized by the product of the imaginary atom-dimer coupling and the $p$-wave effective range. Our results indicate that for a given imaginary atom-dimer coupling, a smaller magnitude of the effective ranges of $p$-wave interaction is crucial for reaching the non-Hermitian $p$-wave Fermi superfluid state.
title Non-Hermitian $p$-wave superfluid and effects of the inelastic three-body loss in a one-dimensional spin-polarized Fermi gas
topic Quantum Gases
Strongly Correlated Electrons
Superconductivity
Nuclear Theory
Quantum Physics
url https://arxiv.org/abs/2312.15724