2014
DOI: 10.1063/1.4903140
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Relaxation dynamics in correlated quantum dots

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Cited by 3 publications
(2 citation statements)
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“…Specifically, we investigate the nonequilibrium steady state dynamics of a SIAM, which is driven by the coupling to two leads at different chemical potentials, caused by an external bias voltage φ. Impurity models in such a setup were considered already by many groups, numerically as well as analytically. [38][39][40] To give a brief non-exhaustive overview, different techniques employed are the noncrossing approximation, [41][42][43] real-time diagrammatic methods, 44 Keldysh perturbation theory, 45 Keldysh effective field theory, 46,47 dual fermions, 48,49 perturbative RG, 50,51 flow equations, 52,53 functional RG, 54,55 real-time RG, [56][57][58][59] time-dependent density matrix RG, [60][61][62][63] NRG, [64][65][66] Monte Carlo methods, [67][68][69] as well as cluster approaches. 70 The properties of the correlated impurity have been established in certain limits, for example for high temperatures T ≫ T K or high biases φ ≫ T K , where the Kondo effect is strongly suppressed by decoherence and the problem reduces to a weak coupling one.…”
Section: Introductionmentioning
confidence: 99%
“…Specifically, we investigate the nonequilibrium steady state dynamics of a SIAM, which is driven by the coupling to two leads at different chemical potentials, caused by an external bias voltage φ. Impurity models in such a setup were considered already by many groups, numerically as well as analytically. [38][39][40] To give a brief non-exhaustive overview, different techniques employed are the noncrossing approximation, [41][42][43] real-time diagrammatic methods, 44 Keldysh perturbation theory, 45 Keldysh effective field theory, 46,47 dual fermions, 48,49 perturbative RG, 50,51 flow equations, 52,53 functional RG, 54,55 real-time RG, [56][57][58][59] time-dependent density matrix RG, [60][61][62][63] NRG, [64][65][66] Monte Carlo methods, [67][68][69] as well as cluster approaches. 70 The properties of the correlated impurity have been established in certain limits, for example for high temperatures T ≫ T K or high biases φ ≫ T K , where the Kondo effect is strongly suppressed by decoherence and the problem reduces to a weak coupling one.…”
Section: Introductionmentioning
confidence: 99%
“…Introduction -Since the times of Kondo [1] and Anderson [2], physicists have been fascinated by the possible effects of embedding a correlated quantum impurity in a metallic host [3][4][5][6]. Recently, a lot of work in this area has also concentrated around the Interacting Resonant Level model (IRLM) [7][8][9][10][11][12][13][14][15][16][17][18][19][20][21][22]; first introduced in 1978 [7] as formally equivalent to the anisotropic Kondo model, it gained a lot of interest in its own right since various exact solutions out of equilibrium were proposed for it [13][14][15]. Despite a lot of progress being made on non-equilibrium transport in the IRLM [8][9][10][11][12][13][14][15][16][17][18][19][20][21][22], there remains open questions about equilibrium properties.…”
mentioning
confidence: 99%