2014
DOI: 10.1103/physrevb.90.241108
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Phase diagram and excitations of a Shiba molecule

Abstract: We analyze the phase diagram associated with a pair of magnetic impurities trapped in a superconducting host. The natural interplay between Kondo screening, superconductivity and exchange interactions leads to a rich array of competing phases, whose transitions are characterized by discontinuous changes of the total spin. Our analysis is based on a combination of numerical renormalization group techniques as well as semi-classical analytics. In addition to the expected screened and unscreened phases, we observ… Show more

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Cited by 49 publications
(44 citation statements)
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References 45 publications
(58 reference statements)
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“…The complexity of crystal-field splitting [19,20], vibrational degrees of freedom [21], spinorbit coupling [22][23][24][25], temperature [26], or external magnetic fields [20] have also been included into the theoretical treatments of single impurities. Theoretical models also discussed the coupling of two magnetic impurities long before their experimental observation [27][28][29][30][31][32][33][34]. Finally, the theoretical considerations expanded on the coupling of magnetic impurities into one-dimensional chains and led to the prediction of Majorana bound states for helical [35,36] and ferromagnetic chains [37,38].…”
mentioning
confidence: 99%
“…The complexity of crystal-field splitting [19,20], vibrational degrees of freedom [21], spinorbit coupling [22][23][24][25], temperature [26], or external magnetic fields [20] have also been included into the theoretical treatments of single impurities. Theoretical models also discussed the coupling of two magnetic impurities long before their experimental observation [27][28][29][30][31][32][33][34]. Finally, the theoretical considerations expanded on the coupling of magnetic impurities into one-dimensional chains and led to the prediction of Majorana bound states for helical [35,36] and ferromagnetic chains [37,38].…”
mentioning
confidence: 99%
“…The proximity of SC induces pairing in QDs [41,42] and tends to suppress the Kondo effect if the superconducting energy gap 2∆ becomes larger than the relevant Kondo temperature T K [40,[43][44][45][46][47][48][49]. Moreover, the strength of SC pairing can greatly affect the Kondo physics in the sub-gap transport regime: For QDs attached to SC and normal contacts, it can enhance the Kondo effect [50][51][52], while for DQD-based Cooper pair splitters, it tends to suppress both the SU(2) and SU(4) Kondo effects [53].…”
Section: Nanostructuresmentioning
confidence: 99%
“…Nevertheless, the phase transition does manifest as a visible spectral discontinuity: there is a kink in the energy of the doublet excitation, and the spectral weights have a jump (results not shown). Alternatively, the radio-frequency spectroscopy could be used 34 . The two-impurity Kondo effect quantum phase transition is thus in principle spectroscopically observable, if only a system with sufficiently suppressed particle exchange could be physically realized 73 .…”
Section: Two-impurity Kondo "Criticality"mentioning
confidence: 99%