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notice that V2 =2D/π results in perfect transmission through the upper arm of the ring [see Eq. 2].
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at zero-temperature, the real part of the GF is calculated either directly from the Lehman representation or performing a Kramers-Kronig transformation. We use NRG parameter Λ=2.5, logarithmic broadening to calculate the spectral function, and keep 1000 states.
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at zero-temperature, the real part of the GF is calculated either directly from the Lehman representation or performing a Kramers-Kronig transformation. We use NRG parameter Λ=2.5, logarithmic broadening to calculate the spectral function, and keep 1000 states.
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34
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68949162664
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Detailed studies of the asymmetry in the LDOS for high |ω| (TK) require the use of generalized NRG techniques;
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Detailed studies of the asymmetry in the LDOS for high |ω| ( TK) require the use of generalized NRG techniques
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68949154027
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note
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One can show that Δσ (0) = Δ 0 so that the Friedel sum rule for the fully compensated case yields ρ (0) =1/π Δ 0.
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