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) [Eqs. (2) and (3)] must therefore be corrected according to Πel(ω,V)→Πel(ω, V)-Πel(ω=0,V=0), where Πel(ω=0,V=0) is the static zero-bias self-energy, in order not to double count these contributions.
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) [Eqs. (2) and (3)] must therefore be corrected according to Π el (ω, V) → Π el (ω, V) - Π el (ω = 0, V = 0), where Π el (ω = 0, V = 0) is the static zero-bias self-energy, in order not to double count these contributions.
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See Supplemental Material at http://link.aps.org/supplemental/10.1103/ PhysRevB.88.201405 for the details of the theory and the first-principles calculations.
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See Supplemental Material at
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In spite of the nonconservative nature of the first Born approximation applied here, it is expected to give a quantitative description of vibrational heating in the regime of weak el-vib interaction (Ref.).
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In spite of the nonconservative nature of the first Born approximation applied here, it is expected to give a quantitative description of vibrational heating in the regime of weak el-vib interaction (Ref.).
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Our choice of parameters for the OPV3 junction corresponds to a zero-bias conductance of G∼0.1G0 (G0=2e2/h), which is slightly larger than the conductance values reported in Ref..
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Our choice of parameters for the OPV3 junction corresponds to a zero-bias conductance of G ∼ 0.1 G 0 (G 0 = 2 e 2 / h), which is slightly larger than the conductance values reported in Ref..
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Note that the cross section for Raman scattering is mode dependent, implying that not all spectral lines show up in Raman spectroscopy.
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Note that the cross section for Raman scattering is mode dependent, implying that not all spectral lines show up in Raman spectroscopy.
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