Matches in SemOpenAlex for { <https://semopenalex.org/work/W2559792371> ?p ?o ?g. }
- W2559792371 abstract "Parafermionic zero modes are a novel set of excitations displaying non-Abelian statistics somewhat richer than that of Majorana modes. These modes are predicted to occur when nearby fractional quantum Hall edge states are gapped by an interposed superconductor. Despite substantial experimental progress, we argue that the necessary crossed Andreev reflection in this arrangement is a challenging milestone to reach. We propose a superconducting quantum dot array structure on a fractional quantum Hall edge that can lead to parafermionic zero modes from coherent superconducting forward scattering on a quantum Hall edge. Such coherent forward scattering has already been demonstrated in recent experiments. We show that for a spin-singlet superconductor interacting with loops of spin unpolarized $2/3$ fractional quantum edge, even an array size of order ten should allow one to systematically tune into a parafermionic degeneracy." @default.
- W2559792371 created "2016-12-16" @default.
- W2559792371 creator A5032629984 @default.
- W2559792371 creator A5074981073 @default.
- W2559792371 creator A5079196272 @default.
- W2559792371 creator A5083164855 @default.
- W2559792371 date "2017-11-20" @default.
- W2559792371 modified "2023-10-12" @default.
- W2559792371 title "Z3 Parafermionic Zero Modes without Andreev Backscattering from the 2/3 Fractional Quantum Hall State" @default.
- W2559792371 cites W1772104798 @default.
- W2559792371 cites W1858949336 @default.
- W2559792371 cites W1965741196 @default.
- W2559792371 cites W1973972788 @default.
- W2559792371 cites W1980009352 @default.
- W2559792371 cites W2000191305 @default.
- W2559792371 cites W2010878960 @default.
- W2559792371 cites W2013500054 @default.
- W2559792371 cites W2015165083 @default.
- W2559792371 cites W2022245421 @default.
- W2559792371 cites W2022315766 @default.
- W2559792371 cites W2024459022 @default.
- W2559792371 cites W2029248386 @default.
- W2559792371 cites W2037034135 @default.
- W2559792371 cites W2039774900 @default.
- W2559792371 cites W2055424520 @default.
- W2559792371 cites W2067650803 @default.
- W2559792371 cites W2079305833 @default.
- W2559792371 cites W2088300719 @default.
- W2559792371 cites W2115109350 @default.
- W2559792371 cites W2116325781 @default.
- W2559792371 cites W2143174693 @default.
- W2559792371 cites W2152240519 @default.
- W2559792371 cites W2167838187 @default.
- W2559792371 cites W2168226651 @default.
- W2559792371 cites W2262023322 @default.
- W2559792371 cites W2277573220 @default.
- W2559792371 cites W2279456634 @default.
- W2559792371 cites W2296259435 @default.
- W2559792371 cites W2523816484 @default.
- W2559792371 cites W3047351161 @default.
- W2559792371 cites W3103010694 @default.
- W2559792371 cites W3104974453 @default.
- W2559792371 cites W3105320508 @default.
- W2559792371 cites W3105605562 @default.
- W2559792371 cites W3121244370 @default.
- W2559792371 cites W3121302533 @default.
- W2559792371 cites W3125378746 @default.
- W2559792371 doi "https://doi.org/10.1103/physrevlett.119.217701" @default.
- W2559792371 hasPubMedId "https://pubmed.ncbi.nlm.nih.gov/29219409" @default.
- W2559792371 hasPublicationYear "2017" @default.
- W2559792371 type Work @default.
- W2559792371 sameAs 2559792371 @default.
- W2559792371 citedByCount "14" @default.
- W2559792371 countsByYear W25597923712018 @default.
- W2559792371 countsByYear W25597923712019 @default.
- W2559792371 countsByYear W25597923712020 @default.
- W2559792371 countsByYear W25597923712021 @default.
- W2559792371 countsByYear W25597923712022 @default.
- W2559792371 crossrefType "journal-article" @default.
- W2559792371 hasAuthorship W2559792371A5032629984 @default.
- W2559792371 hasAuthorship W2559792371A5074981073 @default.
- W2559792371 hasAuthorship W2559792371A5079196272 @default.
- W2559792371 hasAuthorship W2559792371A5083164855 @default.
- W2559792371 hasBestOaLocation W25597923711 @default.
- W2559792371 hasConcept C121332964 @default.
- W2559792371 hasConcept C136479403 @default.
- W2559792371 hasConcept C145727058 @default.
- W2559792371 hasConcept C147120987 @default.
- W2559792371 hasConcept C184423171 @default.
- W2559792371 hasConcept C191486275 @default.
- W2559792371 hasConcept C200369452 @default.
- W2559792371 hasConcept C26873012 @default.
- W2559792371 hasConcept C2777727622 @default.
- W2559792371 hasConcept C2778761060 @default.
- W2559792371 hasConcept C42704618 @default.
- W2559792371 hasConcept C54101563 @default.
- W2559792371 hasConcept C60644358 @default.
- W2559792371 hasConcept C62520636 @default.
- W2559792371 hasConcept C66870719 @default.
- W2559792371 hasConcept C84114770 @default.
- W2559792371 hasConcept C86803240 @default.
- W2559792371 hasConcept C97355855 @default.
- W2559792371 hasConceptScore W2559792371C121332964 @default.
- W2559792371 hasConceptScore W2559792371C136479403 @default.
- W2559792371 hasConceptScore W2559792371C145727058 @default.
- W2559792371 hasConceptScore W2559792371C147120987 @default.
- W2559792371 hasConceptScore W2559792371C184423171 @default.
- W2559792371 hasConceptScore W2559792371C191486275 @default.
- W2559792371 hasConceptScore W2559792371C200369452 @default.
- W2559792371 hasConceptScore W2559792371C26873012 @default.
- W2559792371 hasConceptScore W2559792371C2777727622 @default.
- W2559792371 hasConceptScore W2559792371C2778761060 @default.
- W2559792371 hasConceptScore W2559792371C42704618 @default.
- W2559792371 hasConceptScore W2559792371C54101563 @default.
- W2559792371 hasConceptScore W2559792371C60644358 @default.
- W2559792371 hasConceptScore W2559792371C62520636 @default.
- W2559792371 hasConceptScore W2559792371C66870719 @default.
- W2559792371 hasConceptScore W2559792371C84114770 @default.
- W2559792371 hasConceptScore W2559792371C86803240 @default.
- W2559792371 hasConceptScore W2559792371C97355855 @default.