Since for the Hamiltonian one hasg (H) − g(H) + − (g(H) 0 )2 =ω 2 eff,Eq

= 2α gg(H) − g(H) + −(g −g+ −g 2 0) ,(S22) 8 where the superscript (H) denotes the coefficients associated withH(t)

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cond-mat.stat-mech · 2026-02-27 · unverdicted · novelty 6.0

In quantum thermalization with detailed balance, internal energy becomes E(S, dot S), extending thermodynamics to include dynamical rates.

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Thermodynamics Beyond State Functions from Quantum Relaxation cond-mat.stat-mech · 2026-02-27 · unverdicted · none · ref 18
In quantum thermalization with detailed balance, internal energy becomes E(S, dot S), extending thermodynamics to include dynamical rates.