Matches in SemOpenAlex for { <https://semopenalex.org/work/W1864199568> ?p ?o ?g. }
- W1864199568 abstract "In the past few years materials with protected gapless surface (edge) states have risen to the central stage of condensed matter physics. Almost all discussions centered around topological insulators and superconductors, which possess full quasiparticle gaps in the bulk. In this paper we argue that systems with topological stable bulk nodes offer another class of materials with robust gapless surface states. Moreover the location of the bulk nodes determines the Miller index of the surfaces that show (or do not show) such states. Measuring the spectroscopic signature of these zero modes allows a phase-sensitive determination of the nodal structures of unconventional superconductors when other phase-sensitive techniques are not applicable. We apply this idea to gapless iron-based superconductors and show how to distinguish accidental from symmetry-dictated nodes. We shall argue that the same idea leads to a method for detecting a class of the elusive spin liquids." @default.
- W1864199568 created "2016-06-24" @default.
- W1864199568 creator A5018430066 @default.
- W1864199568 creator A5042930387 @default.
- W1864199568 date "2012-09-13" @default.
- W1864199568 modified "2023-09-27" @default.
- W1864199568 title "Topological relation between bulk gap nodes and surface bound states: Application to iron-based superconductors" @default.
- W1864199568 cites W1488832765 @default.
- W1864199568 cites W1501955150 @default.
- W1864199568 cites W1566432417 @default.
- W1864199568 cites W1774774861 @default.
- W1864199568 cites W1887477448 @default.
- W1864199568 cites W1897682878 @default.
- W1864199568 cites W1940299161 @default.
- W1864199568 cites W1977967750 @default.
- W1864199568 cites W1981625068 @default.
- W1864199568 cites W1984518889 @default.
- W1864199568 cites W1988549733 @default.
- W1864199568 cites W2003397144 @default.
- W1864199568 cites W2007569352 @default.
- W1864199568 cites W2008761774 @default.
- W1864199568 cites W2011970097 @default.
- W1864199568 cites W2017935103 @default.
- W1864199568 cites W2020332193 @default.
- W1864199568 cites W2024570095 @default.
- W1864199568 cites W2026404112 @default.
- W1864199568 cites W2037074763 @default.
- W1864199568 cites W2043662940 @default.
- W1864199568 cites W2045511877 @default.
- W1864199568 cites W2054787976 @default.
- W1864199568 cites W2065576552 @default.
- W1864199568 cites W2067129152 @default.
- W1864199568 cites W2073208780 @default.
- W1864199568 cites W2074665638 @default.
- W1864199568 cites W2079305833 @default.
- W1864199568 cites W2084899562 @default.
- W1864199568 cites W2092831789 @default.
- W1864199568 cites W2102074887 @default.
- W1864199568 cites W2113228663 @default.
- W1864199568 cites W2149445832 @default.
- W1864199568 cites W2290163007 @default.
- W1864199568 cites W2331297845 @default.
- W1864199568 cites W3023162579 @default.
- W1864199568 cites W3102375756 @default.
- W1864199568 cites W3145021469 @default.
- W1864199568 doi "https://doi.org/10.1103/physrevb.86.094512" @default.
- W1864199568 hasPublicationYear "2012" @default.
- W1864199568 type Work @default.
- W1864199568 sameAs 1864199568 @default.
- W1864199568 citedByCount "31" @default.
- W1864199568 countsByYear W18641995682012 @default.
- W1864199568 countsByYear W18641995682013 @default.
- W1864199568 countsByYear W18641995682014 @default.
- W1864199568 countsByYear W18641995682015 @default.
- W1864199568 countsByYear W18641995682016 @default.
- W1864199568 countsByYear W18641995682017 @default.
- W1864199568 countsByYear W18641995682018 @default.
- W1864199568 countsByYear W18641995682019 @default.
- W1864199568 countsByYear W18641995682021 @default.
- W1864199568 countsByYear W18641995682023 @default.
- W1864199568 crossrefType "journal-article" @default.
- W1864199568 hasAuthorship W1864199568A5018430066 @default.
- W1864199568 hasAuthorship W1864199568A5042930387 @default.
- W1864199568 hasBestOaLocation W18641995682 @default.
- W1864199568 hasConcept C114614502 @default.
- W1864199568 hasConcept C121332964 @default.
- W1864199568 hasConcept C128911142 @default.
- W1864199568 hasConcept C136479403 @default.
- W1864199568 hasConcept C184720557 @default.
- W1864199568 hasConcept C24057170 @default.
- W1864199568 hasConcept C2524010 @default.
- W1864199568 hasConcept C26873012 @default.
- W1864199568 hasConcept C2776799497 @default.
- W1864199568 hasConcept C2779886137 @default.
- W1864199568 hasConcept C33332235 @default.
- W1864199568 hasConcept C33923547 @default.
- W1864199568 hasConcept C44280652 @default.
- W1864199568 hasConcept C45646460 @default.
- W1864199568 hasConcept C54101563 @default.
- W1864199568 hasConcept C62520636 @default.
- W1864199568 hasConcept C79689650 @default.
- W1864199568 hasConcept C84114770 @default.
- W1864199568 hasConceptScore W1864199568C114614502 @default.
- W1864199568 hasConceptScore W1864199568C121332964 @default.
- W1864199568 hasConceptScore W1864199568C128911142 @default.
- W1864199568 hasConceptScore W1864199568C136479403 @default.
- W1864199568 hasConceptScore W1864199568C184720557 @default.
- W1864199568 hasConceptScore W1864199568C24057170 @default.
- W1864199568 hasConceptScore W1864199568C2524010 @default.
- W1864199568 hasConceptScore W1864199568C26873012 @default.
- W1864199568 hasConceptScore W1864199568C2776799497 @default.
- W1864199568 hasConceptScore W1864199568C2779886137 @default.
- W1864199568 hasConceptScore W1864199568C33332235 @default.
- W1864199568 hasConceptScore W1864199568C33923547 @default.
- W1864199568 hasConceptScore W1864199568C44280652 @default.
- W1864199568 hasConceptScore W1864199568C45646460 @default.
- W1864199568 hasConceptScore W1864199568C54101563 @default.
- W1864199568 hasConceptScore W1864199568C62520636 @default.
- W1864199568 hasConceptScore W1864199568C79689650 @default.
- W1864199568 hasConceptScore W1864199568C84114770 @default.