2016
DOI: 10.1103/physrevb.93.085441
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Consistent bosonization-debosonization. II. The two-lead Kondo problem and the fate of its nonequilibrium Toulouse point

Abstract: Following the development of a scheme to bosonize and debosonize consistently [N. Shah and C.J. Bolech, Phys. Rev B 93, 085440 (2016); arXiv:1508.03078], we present in detail the Toulouse-point analytic solution of the two-lead Kondo junction model. The existence and location of the solvable point is not modified, but the calculational methodology and the final expressions for observable quantities change markedly as compared to the existent results. This solvable point is one of the remarkably few exact resu… Show more

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Cited by 15 publications
(12 citation statements)
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References 74 publications
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“…These include the appearance of the peak in the differential conductance around h z ∼ V and the asymmetry between the conductance behavior at V = 0 with varying h z and the one at h z = 0 with varying V . In particular, it has been argued that this asymmetry is an important feature which is absent in the "conventional" bosonization treatment [110]. Yet, there seem to be differences between the asymmetric behavior found in our results and that found in the above reference.…”
Section: Conductance At Finite Bias and Magnetic Fieldcontrasting
confidence: 90%
See 1 more Smart Citation
“…These include the appearance of the peak in the differential conductance around h z ∼ V and the asymmetry between the conductance behavior at V = 0 with varying h z and the one at h z = 0 with varying V . In particular, it has been argued that this asymmetry is an important feature which is absent in the "conventional" bosonization treatment [110]. Yet, there seem to be differences between the asymmetric behavior found in our results and that found in the above reference.…”
Section: Conductance At Finite Bias and Magnetic Fieldcontrasting
confidence: 90%
“…We analyze out-of-equilibrium dynamics and transport properties in the two-lead Kondo model and demonstrate that our approach can be used to compute the long-time spatiotemporal dynamics and the conductance at finite bias and magnetic field. The obtained results are consistent with the previous studies in the Anderson model [88,99,114] and the exact solutions at the Toulouse point [110].…”
Section: Introductionsupporting
confidence: 93%
“…The tunneling across the classically forbidden region is modeled by a tight-binding matrix overlap γt that can be taken to be energy independent in certain cases (in particular, the characteristic energy scale of dependence of the transmission coefficient, |γt| 2 , has to be much larger than both eV and kBT [8]). Here we assume that the barrier region does not allow for internal states; a situation when that happens will be discussed elsewhere [16].…”
Section: A Setting Of the Problem And Direct Solutionmentioning
confidence: 99%
“…In the future we will look at more involved examples of greater physical significance. We already started to reexamine some salient cases, and in the next paper we shall focus on the important case of transport through quantum impurities in Fermi liquids [16].…”
Section: Conclusion and Prospectsmentioning
confidence: 99%
“…Specifically, exact solutions [13][14][15][16][17][18] at the Toulouse point of nonequilibrium Kondo models are inapplicable to the more microscopic Anderson model. Quantum Monte Carlo [19][20][21][22] and master equation [23][24][25][26][27] methods cannot access the strong-coupling Kondo limit at zero temperature.…”
Section: Introductionmentioning
confidence: 99%