Markovian state dynamics are thermodynamically incomplete because reservoir-channel assignments can vary while leaving the master equation unchanged, yielding different heat currents, entropy production, and noise.
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Derives a Boltzmann-like distribution over actions via maximum entropy subject to a mean-action constraint, producing a Markovian stochastic propagator that matches Brownian motion and remains covariant at relativistic speeds.
A second-order perturbative framework decomposes coherence terms in the quantum first law into coherent heat and work, linking them to Fermi's golden rule transition rates.
citing papers explorer
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Thermodynamic incompleteness of state dynamics in Markovian transport
Markovian state dynamics are thermodynamically incomplete because reservoir-channel assignments can vary while leaving the master equation unchanged, yielding different heat currents, entropy production, and noise.
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Stochastic dynamics from maximum entropy in action space
Derives a Boltzmann-like distribution over actions via maximum entropy subject to a mean-action constraint, producing a Markovian stochastic propagator that matches Brownian motion and remains covariant at relativistic speeds.
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Perturbative approach to the first law of quantum thermodynamics
A second-order perturbative framework decomposes coherence terms in the quantum first law into coherent heat and work, linking them to Fermi's golden rule transition rates.