Criticality in the Crossed Andreev Reflection of a Quantum Hall Edge

We develop a theory of the nonlocal transport of two counterpropagating ν=1 quantum Hall edges coupled via a narrow disordered superconductor. Contrary to the predictions developed for the clean case, the edge states proximitized in this way do not turn into a topological superconductor. Instead, th...

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Main Authors: Vladislav D. Kurilovich, Leonid I. Glazman
Format: Article
Language:English
Published: American Physical Society 2023-09-01
Series:Physical Review X
Online Access:http://doi.org/10.1103/PhysRevX.13.031027
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author Vladislav D. Kurilovich
Leonid I. Glazman
author_facet Vladislav D. Kurilovich
Leonid I. Glazman
author_sort Vladislav D. Kurilovich
collection DOAJ
description We develop a theory of the nonlocal transport of two counterpropagating ν=1 quantum Hall edges coupled via a narrow disordered superconductor. Contrary to the predictions developed for the clean case, the edge states proximitized in this way do not turn into a topological superconductor. Instead, they are naturally tuned to the critical point between trivial and topological phases. This occurs due to the competition between tunneling processes with and without particle-hole conversion. The critical conductance is a random, sample-specific quantity with a zero average and unusual bias dependence. The negative values of conductance are relatively stable against variations of the carrier density, which may make the critical state appear as a topological one. Our results offer an interpretation of recent experiments [G.-H. Lee et al., Nat. Phys. 13, 693 (2017)NPAHAX1745-247310.1038/nphys4084; O. Gül et al., Phys. Rev. X 12, 021057 (2022)PRXHAE2160-330810.1103/PhysRevX.12.021057].
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spelling doaj.art-ab8be2a0a0df4803ac6ffb556e0ca8822023-09-12T14:54:12ZengAmerican Physical SocietyPhysical Review X2160-33082023-09-0113303102710.1103/PhysRevX.13.031027Criticality in the Crossed Andreev Reflection of a Quantum Hall EdgeVladislav D. KurilovichLeonid I. GlazmanWe develop a theory of the nonlocal transport of two counterpropagating ν=1 quantum Hall edges coupled via a narrow disordered superconductor. Contrary to the predictions developed for the clean case, the edge states proximitized in this way do not turn into a topological superconductor. Instead, they are naturally tuned to the critical point between trivial and topological phases. This occurs due to the competition between tunneling processes with and without particle-hole conversion. The critical conductance is a random, sample-specific quantity with a zero average and unusual bias dependence. The negative values of conductance are relatively stable against variations of the carrier density, which may make the critical state appear as a topological one. Our results offer an interpretation of recent experiments [G.-H. Lee et al., Nat. Phys. 13, 693 (2017)NPAHAX1745-247310.1038/nphys4084; O. Gül et al., Phys. Rev. X 12, 021057 (2022)PRXHAE2160-330810.1103/PhysRevX.12.021057].http://doi.org/10.1103/PhysRevX.13.031027
spellingShingle Vladislav D. Kurilovich
Leonid I. Glazman
Criticality in the Crossed Andreev Reflection of a Quantum Hall Edge
Physical Review X
title Criticality in the Crossed Andreev Reflection of a Quantum Hall Edge
title_full Criticality in the Crossed Andreev Reflection of a Quantum Hall Edge
title_fullStr Criticality in the Crossed Andreev Reflection of a Quantum Hall Edge
title_full_unstemmed Criticality in the Crossed Andreev Reflection of a Quantum Hall Edge
title_short Criticality in the Crossed Andreev Reflection of a Quantum Hall Edge
title_sort criticality in the crossed andreev reflection of a quantum hall edge
url http://doi.org/10.1103/PhysRevX.13.031027
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