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Main Authors: Zhu, Pingcheng, Zhou, Lihong, Zhong, Jianxin
Format: Preprint
Published: 2026
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Online Access:https://arxiv.org/abs/2601.01790
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author Zhu, Pingcheng
Zhou, Lihong
Zhong, Jianxin
author_facet Zhu, Pingcheng
Zhou, Lihong
Zhong, Jianxin
contents The experimental advances in realizing artificial spin-orbit coupling (SOC) and non-Hermitian potentials in ultracold atomic system open a new avenue for exploring their significant roles in quantum many-body physics. Here, we investigate a non-Hermitian, two-component Fermi system in a cubic lattice with Rashba SOC and complex-valued interaction arising from two-body loss. We adopt the non-Hermitian mean field theory and map out the phase diagram at zero temperature. The interplay of dissipation and on-site interaction drives a dissipation-induced phase transition from superfluid (SF) to normal phase (N). Notably, for weak interaction strengths, this leads to a reentrance of the superfluid state. The presence of SOC significantly expands the parameter regime for both the normal phase and the metastable superfluid phase(MSF). Whereas, the Zeeman field can drive the system from a conventional superfluid into a topological superfluid phase(TSF), characterized by a nontrivial topological invariant. These results enrich our knowledge of pairing superfluidity in Fermi systems.
format Preprint
id arxiv_https___arxiv_org_abs_2601_01790
institution arXiv
publishDate 2026
record_format arxiv
spellingShingle Non-Hermitian topological superfluidity in a three-dimensional fermi gas with spin-orbit coupling
Zhu, Pingcheng
Zhou, Lihong
Zhong, Jianxin
Quantum Gases
The experimental advances in realizing artificial spin-orbit coupling (SOC) and non-Hermitian potentials in ultracold atomic system open a new avenue for exploring their significant roles in quantum many-body physics. Here, we investigate a non-Hermitian, two-component Fermi system in a cubic lattice with Rashba SOC and complex-valued interaction arising from two-body loss. We adopt the non-Hermitian mean field theory and map out the phase diagram at zero temperature. The interplay of dissipation and on-site interaction drives a dissipation-induced phase transition from superfluid (SF) to normal phase (N). Notably, for weak interaction strengths, this leads to a reentrance of the superfluid state. The presence of SOC significantly expands the parameter regime for both the normal phase and the metastable superfluid phase(MSF). Whereas, the Zeeman field can drive the system from a conventional superfluid into a topological superfluid phase(TSF), characterized by a nontrivial topological invariant. These results enrich our knowledge of pairing superfluidity in Fermi systems.
title Non-Hermitian topological superfluidity in a three-dimensional fermi gas with spin-orbit coupling
topic Quantum Gases
url https://arxiv.org/abs/2601.01790