2015
DOI: 10.1103/physrevb.91.245158
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Density functional description of Coulomb blockade: Adiabatic versus dynamic exchange correlation

Abstract: Above the Kondo temperature, the Kohn-Sham zero-bias conductance of an Anderson junction has been shown to completely miss the Coulomb blockade. Within a standard model for the spectral function, we deduce a parameterization for both the onsite exchange-correlation potential and the bias drop as a function of the site occupation that applies for all correlation strengths. We use our results to sow doubt on the common interpretation of such corrections as arising from dynamical exchange-correlation contribution… Show more

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Cited by 12 publications
(9 citation statements)
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“…We emphasize that this polarization is not physically correct as the system has unpolarized leads -hence the chemical potentials for both spin directions are identical. However, it has been pointed out by several researchers that the spin-polarized states found in DFT calculations can give us valuable information about the levels and their occupation 11,[44][45][46] .…”
Section: Image Charge Effects For Benzenediamine (Bda)mentioning
confidence: 99%
“…We emphasize that this polarization is not physically correct as the system has unpolarized leads -hence the chemical potentials for both spin directions are identical. However, it has been pointed out by several researchers that the spin-polarized states found in DFT calculations can give us valuable information about the levels and their occupation 11,[44][45][46] .…”
Section: Image Charge Effects For Benzenediamine (Bda)mentioning
confidence: 99%
“…The electronic transport has also been studied by applying SOFT to the Anderson junction model [46][47][48]. Time-dependent [49][50][51] and temperature-dependent extensions [52,53] have been investigated over the years.…”
Section: Introductionmentioning
confidence: 99%
“…when both sites are half-filled) in the strongly correlated limit (U/t → +∞). A similar discontinuity can be observed in the Anderson junction model [55][56][57]. It can be interpreted as follows: the impurity site with occupation n is an open system and, in order to let n vary continuously from 0 to 1, we need a grand canonical ensemble consisting of degenerate zero-and one-electron states.…”
Section: Embedded Impurity Systemmentioning
confidence: 63%