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• W2023444851 abstract "In momentum space the time-ordered, retarded, and Feynman thermal propagators all satisfy rather simple dispersion relations. In coordinate space the first two propagators are related to the thermal Wightman function Tr[ensuremath{varphi}(x)ensuremath{varphi}(0)${mathit{e}}^{mathrm{ensuremath{-}}mathrm{ensuremath{beta}}mathit{H}}$]. However, the Feynman thermal propagator in coordinate space, ${mathit{D}}_{mathit{F}}$(x), is not related to this thermal average and does not satisfy a KMS condition in complex time. When expressed in terms of matrix elements of the field operator, it requires a new type of operator ordering. textcopyright{} 1996 The American Physical Society." @default.
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• W2023444851 date "1996-06-15" @default.
• W2023444851 modified "2023-10-16" @default.
• W2023444851 title "Finite-temperature Feynman propagator in operator form" @default.
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• W2023444851 doi "https://doi.org/10.1103/physrevd.53.7265" @default.
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