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This paper investigates the non-equilibrium dynamics of spinless fermions under dephasing noise using a many-particle Lindblad equation framework. By mapping these systems to an exactly solvable Hubbard model with imaginary tunneling amplitude, it reveals how quartic operators generate interacting hydrodynamic modes and distinct late-time diffusive tails not predicted by standard symmetry constraints alone. These findings advance the theoretical understanding of open quantum systems where noise fundamentally alters transport properties beyond simple bilinear approximations.
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Interacting hydrodynamic modes in spinless fermions with dephasing noise

arXiv2 min read

arXiv:2607.25938v1 Announce Type: cross Abstract: We study the non-equilibrium dynamics of spinless fermions with dephasing noise in the framework of a many-particle Lindblad equation. Using a mapping to the exactly solvable one-dimensional Hubbard model with purely imaginary tunneling amplitude we analyze the Heisenberg-picture dynamics of operators quartic in fermions and determine their hydrodynamic projections. We construct the relevant diffusive eigenoperators explicitly and show that, in the quartic sector, they can be interpreted as interacting pairs of bilinear hydrodynamic modes. As a consequence, translationally invariant quartic operators generically exhibit non-vanishing diffusive late-time tails, unlike translationally invariant bilinears. Our results show that the hydrodynamic tails of microscopic operators cannot in general be inferred from symmetry constraints or coarse-grained fluctuating hydrodynamics alone; they also depend crucially on the spatial structure and effective size of the hydrodynamic eigenoperators.

Abstract:We study the non-equilibrium dynamics of spinless fermions with dephasing noise in the framework of a many-particle Lindblad equation. Using a mapping to the exactly solvable one-dimensional Hubbard model with purely imaginary tunneling amplitude we analyze the Heisenberg-picture dynamics of operators quartic in fermions and determine their hydrodynamic projections. We construct the relevant diffusive eigenoperators explicitly and show that, in the quartic sector, they can be interpreted as interacting pairs of bilinear hydrodynamic modes. As a consequence, translationally invariant quartic operators generically exhibit non-vanishing diffusive late-time tails, unlike translationally invariant bilinears. Our results show that the hydrodynamic tails of microscopic operators cannot in general be inferred from symmetry constraints or coarse-grained fluctuating hydrodynamics alone; they also depend crucially on the spatial structure and effective size of the hydrodynamic eigenoperators.

Statistical Mechanics (cond-mat.stat-mech); Quantum Physics (quant-ph)

arXiv:2607.25938 [cond-mat.stat-mech]

(or arXiv:2607.25938v1 [cond-mat.stat-mech] for this version)

https://doi.org/10.48550/arXiv.2607.25938 Focus to learn more arXiv-issued DOI via DataCite (pending registration)

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Full text under the publisher's open licence · 226 words

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