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Imaginary Gauge Potentials in a Non-Hermitian Spin-Orbit Coupled Quantum Gas

J. Tao1,2,*, E. D. Mercado-Gutierrez1,*, M. Zhao1, and I. B. Spielman1,†

  • *These authors contributed equally to this work.
  • †Contact author: ian.spielman@nist.gov

Phys. Rev. Lett. 136, 113401 – Published 17 March, 2026

DOI: https://doi.org/10.1103/tpfc-n3bq

Abstract

In 1996, Hatano and Nelson proposed a non-Hermitian lattice model containing an imaginary Peierls phase [Phys. Rev. Lett. 77, 570 (1996)], which subsequent analyses revealed to be an instance of a new class of topological systems. Here, we experimentally realize a continuum analog to this model containing an imaginary gauge potential using a homogeneous spin-orbit coupled Bose-Einstein condensate (BEC). Non-Hermiticity is introduced by adding tunable spin-dependent loss via microwave coupling to a subspace with spontaneous emission. We demonstrate that the resulting Heisenberg equations of motion for position and momentum depend explicitly on the system’s phase-space distribution. First, we observe collective nonreciprocal transport in real space, with a “self-acceleration” that decreases with the BEC’s spatial extent, consistent with non-Hermitian Gross-Pitaevskii simulations. We then examine localized edge states: the relatively strong interactions in our BEC suppress the formation of topological edge states, yielding instead highly excited states localized by an interplay between self-acceleration and wave function spreading. Finally, we confirm that our non-Hermitian description remains valid at all times by comparing it to a multilevel master equation treatment.

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