Derives ⟨exp(−βX)⟩ = 1 for adiabatic processes to obtain inequalities for the strong thermodynamic bound W ≥ ΔE_S, with classical and quantum versions.
Kasuga, On the adiabatic theorem for the Hamiltonian system of di fferential equations in the classical mechanics, III, Proc
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Fluctuation relations and strong inequalities for thermally isolated systems
Derives ⟨exp(−βX)⟩ = 1 for adiabatic processes to obtain inequalities for the strong thermodynamic bound W ≥ ΔE_S, with classical and quantum versions.