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Several different conventions exist for the definition of the Keldysh structure of the Green's functions. Here we use the convention of Eqs. (2.26) and (2.27) in Ref..
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59649117674
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To derive this equation from the full theory as presented in Ref., the tunneling limit must be taken. This boils down to using Eq. (14) of Ref. instead of the more general Eq. (36).
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To derive this equation from the full theory as presented in Ref., the tunneling limit must be taken. This boils down to using Eq. (14) of Ref. instead of the more general Eq. (36).
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36
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59649123490
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cf. Eqs. (36) and (37) of Ref..
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cf. Eqs. (36) and (37) of Ref..
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37
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59649096342
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While our numerical scheme breaks down when 0< ETh ≪ Δ0, it is again possible to do numerics when the system is perfectly isolated, i.e., when ETh is strictly zero.
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While our numerical scheme breaks down when 0< ETh ≪ Δ0, it is again possible to do numerics when the system is perfectly isolated, i.e., when ETh is strictly zero.
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