Matches in SemOpenAlex for { <https://semopenalex.org/work/W3150819931> ?p ?o ?g. }
- W3150819931 abstract "Magnetic impurities in a superconductor induce Yu-Shiba-Rusinov (YSR) states inside the superconducting gap, whose energy depends on the strength of the coupling to the impurity and on the density of states (DOS) at the Fermi level. We consider DOS exhibiting a logarithmic or a power-law divergence at the Fermi level due to Van Hove singularities (VHS) and high-order Van Hove singularities (HOVHS), respectively. We find that the energy of the YSR states has the same functional form as in the constant DOS scenario, with the effect of the singularity being an enhancement of the effective coupling constants. In particular, the critical magnetic coupling strength at which the Shiba transition occurs is always lowered by a factor $1/rho(Delta/E_{mathrm{c}}$), where $Delta$ is the superconducting gap, $E_{mathrm{c}}$ is the bandwidth, and $rho(E)$ is the factor in DOS which diverges at $E=0$ for a VHS or HOVHS. Further, since the critical magnetic coupling is significantly reduced, a new regime becomes accessible where the transition point is controlled by the non-magnetic coupling constant. Interestingly, the slope of the Shiba energy curve at the Shiba transition is independent of impurity parameters and purely reflects the band structure. Additionally, we find that our main conclusions remain valid even when the Fermi level is not precisely tuned to the Van Hove singularity, but instead lies on an energy range of order the superconducting gap. Our results show that tuning a superconducting material towards a VHS or HOVHS enhances the possibilities for engineering YSR states, and for characterizing the superconductor itself." @default.
- W3150819931 created "2021-04-13" @default.
- W3150819931 creator A5003711223 @default.
- W3150819931 creator A5038184318 @default.
- W3150819931 creator A5062139967 @default.
- W3150819931 date "2021-06-17" @default.
- W3150819931 modified "2023-10-18" @default.
- W3150819931 title "Effect of Van Hove singularities on Shiba states in two-dimensional<mml:math xmlns:mml=http://www.w3.org/1998/Math/MathML><mml:mi>s</mml:mi></mml:math>-wave superconductors" @default.
- W3150819931 cites W1716811706 @default.
- W3150819931 cites W1791667550 @default.
- W3150819931 cites W1809744950 @default.
- W3150819931 cites W1966879286 @default.
- W3150819931 cites W1981581137 @default.
- W3150819931 cites W2000693525 @default.
- W3150819931 cites W2007074937 @default.
- W3150819931 cites W2007298716 @default.
- W3150819931 cites W2010546414 @default.
- W3150819931 cites W2014615332 @default.
- W3150819931 cites W2015312385 @default.
- W3150819931 cites W2015938701 @default.
- W3150819931 cites W2039889589 @default.
- W3150819931 cites W2043828720 @default.
- W3150819931 cites W2044884775 @default.
- W3150819931 cites W2049433350 @default.
- W3150819931 cites W2053093277 @default.
- W3150819931 cites W2055442979 @default.
- W3150819931 cites W2056830045 @default.
- W3150819931 cites W2089843538 @default.
- W3150819931 cites W2092541833 @default.
- W3150819931 cites W2099022785 @default.
- W3150819931 cites W2137096678 @default.
- W3150819931 cites W2140331670 @default.
- W3150819931 cites W2162830063 @default.
- W3150819931 cites W2253377585 @default.
- W3150819931 cites W2267957601 @default.
- W3150819931 cites W2283122682 @default.
- W3150819931 cites W2340442648 @default.
- W3150819931 cites W2480181223 @default.
- W3150819931 cites W2523314206 @default.
- W3150819931 cites W2554178941 @default.
- W3150819931 cites W2742975428 @default.
- W3150819931 cites W2757083356 @default.
- W3150819931 cites W2762484852 @default.
- W3150819931 cites W2793369479 @default.
- W3150819931 cites W2800582642 @default.
- W3150819931 cites W2810503782 @default.
- W3150819931 cites W2901629900 @default.
- W3150819931 cites W2948535855 @default.
- W3150819931 cites W2964212568 @default.
- W3150819931 cites W2982265255 @default.
- W3150819931 cites W2994091299 @default.
- W3150819931 cites W3036374946 @default.
- W3150819931 cites W3095561098 @default.
- W3150819931 cites W3099082337 @default.
- W3150819931 cites W3101074194 @default.
- W3150819931 cites W3101860842 @default.
- W3150819931 cites W3102292770 @default.
- W3150819931 cites W3103450160 @default.
- W3150819931 cites W3120763523 @default.
- W3150819931 cites W3122825682 @default.
- W3150819931 cites W3125280860 @default.
- W3150819931 cites W3126921591 @default.
- W3150819931 cites W3127466677 @default.
- W3150819931 cites W3134043443 @default.
- W3150819931 cites W3154916187 @default.
- W3150819931 cites W4231446668 @default.
- W3150819931 cites W809430256 @default.
- W3150819931 doi "https://doi.org/10.1103/physrevb.103.214514" @default.
- W3150819931 hasPublicationYear "2021" @default.
- W3150819931 type Work @default.
- W3150819931 sameAs 3150819931 @default.
- W3150819931 citedByCount "4" @default.
- W3150819931 countsByYear W31508199312022 @default.
- W3150819931 countsByYear W31508199312023 @default.
- W3150819931 crossrefType "journal-article" @default.
- W3150819931 hasAuthorship W3150819931A5003711223 @default.
- W3150819931 hasAuthorship W3150819931A5038184318 @default.
- W3150819931 hasAuthorship W3150819931A5062139967 @default.
- W3150819931 hasBestOaLocation W31508199312 @default.
- W3150819931 hasConcept C121332964 @default.
- W3150819931 hasConcept C12843 @default.
- W3150819931 hasConcept C131584629 @default.
- W3150819931 hasConcept C144255511 @default.
- W3150819931 hasConcept C147120987 @default.
- W3150819931 hasConcept C183276030 @default.
- W3150819931 hasConcept C191897082 @default.
- W3150819931 hasConcept C192562407 @default.
- W3150819931 hasConcept C26057338 @default.
- W3150819931 hasConcept C26873012 @default.
- W3150819931 hasConcept C40636707 @default.
- W3150819931 hasConcept C53964469 @default.
- W3150819931 hasConcept C54101563 @default.
- W3150819931 hasConcept C62520636 @default.
- W3150819931 hasConceptScore W3150819931C121332964 @default.
- W3150819931 hasConceptScore W3150819931C12843 @default.
- W3150819931 hasConceptScore W3150819931C131584629 @default.
- W3150819931 hasConceptScore W3150819931C144255511 @default.
- W3150819931 hasConceptScore W3150819931C147120987 @default.
- W3150819931 hasConceptScore W3150819931C183276030 @default.
- W3150819931 hasConceptScore W3150819931C191897082 @default.