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    Thermal liquid-gas phase transition in a quasi-one-dimensional dipolar Fermi gas

    Lanxuan Gao1,*,†, Koki Takayama1,*, Hiroyuki Tajima2,3,4, Takahiro M. Doi5,6, and Haozhao Liang2,4,6

    • *These authors contributed equally to this work.
    • †Contact author: gao-lanxuan102@g.ecc.u-tokyo.ac.jp

    Phys. Rev. A 113, 063307 – Published 4 June, 2026

    DOI: https://doi.org/10.1103/z4wr-f6wd

    Abstract

    We theoretically investigate the thermodynamic properties of a quasi-one-dimensional single-component dipolar Fermi gas at finite temperatures. A self-bound fermionic droplet can be achieved by exchange correlations with long-range dipole-dipole interactions under quasi-one-dimensional confinement, where the interaction can be tuned by tilting the dipoles along the system coordinate. Using the Hartree-Fock approximation, we show how the liquid-gas phase transition occurs in this system and elucidate the finite-temperature phase structure consisting of a gas phase, liquid phase, gas-liquid coexistence phase, and spinodal phase. We also discuss its similarity to the liquid-gas phase transition in nuclear matter through a comparison with phenomenological models. By examining the experimental conditions for realizing self-bound fermionic droplets, we find that microwave-shielded fermionic polar molecules are promising candidates. Our results will be useful for an interdisciplinary understanding of self-bound fermionic matter as well as an analog quantum simulation of nuclear systems.

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