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.
If [H, σ] = 0, then the relative entropy with respect toσis invariant under the unitary flow: D e−itH ρeitH ∥σ =D(ρ∥σ).(D1) We differentiate Eq
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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.