2014
DOI: 10.1103/physrevb.90.035426
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Kondo effect in graphene with Rashba spin-orbit coupling

Abstract: We study the Kondo screening of a magnetic impurity adsorbed in graphene in the presence of Rashba spin-orbit interaction. The system is described by an effective single-channel Anderson impurity model, which we analyze using the numerical renormalization group. The nontrivial energy dependence of the host density of states gives rise to interesting behaviors under variation of the chemical potential or the spin-orbit coupling. Varying the Rashba coupling produces strong changes in the Kondo temperature charac… Show more

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Cited by 41 publications
(74 citation statements)
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“…The influence of the SOI on the Kondo effect in 2d TIs has been addressed in several numerical works [28][29][30][31][32] , particularly focusing on the behavior of the Kondo temperature. In overall agreement with Ref.…”
Section: Introductionmentioning
confidence: 99%
“…The influence of the SOI on the Kondo effect in 2d TIs has been addressed in several numerical works [28][29][30][31][32] , particularly focusing on the behavior of the Kondo temperature. In overall agreement with Ref.…”
Section: Introductionmentioning
confidence: 99%
“…Our results show that the Kondo temperature for a substitutional impurity at a crest site is very weakly enhanced by the introduction of SOI, in agreement with numerical renormalization-group calculations of a similar problem [201,203]. For a adatom crest impurity, E corr contrastingly decreases with the SOI.…”
Section: Discussionsupporting
confidence: 74%
“…Unlike prior work by Zarea et al [202] that predicts an exponential enhancement of the Kondo temperature in the presence of SOI, we find that this enhancement is very weak, in agreement with numerical renormalization-group treatments of this problem [201,203]. First, the correlations are considerably larger (in magnitude) for a crest site than for a trough site.…”
Section: Spin Correlations and Kondo Temperature 731 Substitutionalcontrasting
confidence: 28%
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