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This paper establishes an exact theoretical framework for heat, energy, and particle transport in non-Markovian open Gaussian quantum systems using full counting statistics. The approach resolves out-of-equilibrium transient dynamics across arbitrary coupling strengths and applies to both fermionic and bosonic reservoirs, recovering standard Landauer-Büttiker results in the weak-coupling limit. A key finding is the identification of transient negative heat conductance regimes driven by initial state preparation, offering new insights into non-trivial quantum transport phenomena.
Exact quantum transport in non-Markovian open Gaussian systems
arXiv:2602.21190v2 Announce Type: replace Abstract: We build an exact framework to evaluate heat, energy, and particle transport between Gaussian reservoirs mediated by a quadratic quantum system. By combining full counting statistics with newly developed non-Markovian master equation approaches, we introduce an effective master equation whose solution can be used to generate arbitrary moments of the heat statistics for any number of reservoirs. This theory applies equally to fermionic and bosonic systems, holds at arbitrarily strong coupling, and resolves out-of-equilibrium transient dynamics determined by the system's initial state. In the steady-state, weak-coupling limit, we recover results analogous to those of the well-known Landauer-B\"{u}ttiker formalism. We conclude our discussion by demonstrating an application of the method to a prototypical fermionic system. Our results uncover a regime of transient negative heat conductance contingent upon the initial system preparation, providing a clear signature of non-trivial out-of-equilibrium dynamics.
Abstract:We build an exact framework to evaluate heat, energy, and particle transport between Gaussian reservoirs mediated by a quadratic quantum system. By combining full counting statistics with newly developed non-Markovian master equation approaches, we introduce an effective master equation whose solution can be used to generate arbitrary moments of the heat statistics for any number of reservoirs. This theory applies equally to fermionic and bosonic systems, holds at arbitrarily strong coupling, and resolves out-of-equilibrium transient dynamics determined by the system's initial state. In the steady-state, weak-coupling limit, we recover results analogous to those of the well-known Landauer-Büttiker formalism. We conclude our discussion by demonstrating an application of the method to a prototypical fermionic system. Our results uncover a regime of transient negative heat conductance contingent upon the initial system preparation, providing a clear signature of non-trivial out-of-equilibrium dynamics.
Accepted version. 10 pages + 15 pages of appendices, 5 figures
Quantum Physics (quant-ph); Mesoscale and Nanoscale Physics (cond-mat.mes-hall); Statistical Mechanics (cond-mat.stat-mech)
arXiv:2602.21190 [quant-ph]
(or arXiv:2602.21190v2 [quant-ph] for this version)
https://doi.org/10.48550/arXiv.2602.21190 Focus to learn more arXiv-issued DOI via DataCite
Phys. Rev. B 114, 144308 (2026)
https://doi.org/10.1103/577j-lrhg Focus to learn more DOI(s) linking to related resources
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