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- W2018308966 abstract "Starting from the usual formulation of nonequilibrium quantum statistical mechanics, the expectation value of an operator A in a steady state nonequilibrium quantum system is shown to have the form 〈A〉 =Tr{${mathit{e}}^{mathrm{ensuremath{-}}mathrm{ensuremath{beta}}(mathit{H}mathrm{ensuremath{-}}mathit{Y})}$A} /Tr{${mathit{e}}^{mathrm{ensuremath{-}}mathrm{ensuremath{beta}}(mathit{H}mathrm{ensuremath{-}}mathit{Y})}$}, where H is the Hamiltonian, ensuremath{beta} is the inverse of the temperature, and Y is an operator which depends on how the system is driven out of equilibrium. Because 〈A〉 is not expressed as a sum of correlation functions integrated over real time, one can now consider performing nonperturbative calculations in interacting nonequilibrium quantum problems." @default.
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- W2018308966 date "1993-04-05" @default.
- W2018308966 modified "2023-09-27" @default.
- W2018308966 title "Reformulation of steady state nonequilibrium quantum statistical mechanics" @default.
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- W2018308966 doi "https://doi.org/10.1103/physrevlett.70.2134" @default.
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