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Marco Vallone
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More specifically, we define ∫0∞dτeiωτC(τ)=12γ(ω)+iλ(ω). For a bosonic bath with spectral density J(ω) in thermal equilibrium, C(t)=∫0∞dω′J(ω′){[n(ω′)+1]e−iω′t+n(ω′)eiω′t}., where n(ω) is the Bose distribution. This yields γ(ω)∝J(ω)[n(ω)+1] for ω>0 and γ(ω)∝J(|ω|)n(|ω|) for ω<0, while λ(ω) is a principal-value integral over J(ω) (its Hilbert transform). At zero temperature, equations (14) and (15) follow.
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