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0→-∞.
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note
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Historically, the zero-frequency noise (10) contains a factor 2, i.e., S̄′=2S̄, resulting from a different definition of the Fourier transform. Then, the Fano factor is defined as F=S̄′/2e |Ī|.
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57
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A relation similar to Eq. (61) holds also in the time-dependent situation (Ref. 38), cf. Eq. (B8). However, it cannot be used to simplify the zero-frequency noise since in Eq. (45) one energy argument is shifted by kℏhΩ.
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For time-dependent systems, it is possible to generalize the concept of reflection symmetry by taking also time transformations into account (Ref. 59).
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