Bosonic topological insulator intermediate state in the superconductor-insulator transition
•The intervening Bose metal (BM) state is the bosonic topological insulator.•In the bulk vortices and Cooper pairs are frozen by Aharonov-Bohm interactions.•Transport in the Bose metal is mediated by topologically protected edge modes.•Transitions BM–superinsulator and BM–superconductor are quantum...
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Published in | Physics letters. A Vol. 384; no. 23; p. 126570 |
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Main Authors | , , , , , , , , , |
Format | Journal Article |
Language | English |
Published |
Netherlands
Elsevier B.V
17.08.2020
Elsevier |
Subjects | |
Online Access | Get full text |
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Summary: | •The intervening Bose metal (BM) state is the bosonic topological insulator.•In the bulk vortices and Cooper pairs are frozen by Aharonov-Bohm interactions.•Transport in the Bose metal is mediated by topologically protected edge modes.•Transitions BM–superinsulator and BM–superconductor are quantum BKT transitions.
A low-temperature intervening metallic regime arising in the two-dimensional superconductor-insulator transition challenges our understanding of electronic fluids. Here we develop a gauge theory revealing that this emergent anomalous metal is a bosonic topological insulator where bulk transport is suppressed by mutual statistics interactions between out-of-condensate Cooper pairs and vortices and the longitudinal conductivity is mediated by symmetry-protected gapless edge modes. We explore the magnetic-field-driven superconductor-insulator transition in a niobium titanium nitride device and find marked signatures of a bosonic topological insulator behavior of the intervening regime with the saturating resistance. The observed superconductor-anomalous metal and insulator-anomalous metal dual phase transitions exhibit quantum Berezinskii-Kosterlitz-Thouless criticality in accord with the gauge theory. |
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Bibliography: | USDOE Office of Science (SC), Basic Energy Sciences (BES) National Science Foundation (NSF) AC02-06CH11357; DMR-1809188; DMR-1606858 |
ISSN: | 0375-9601 1873-2429 |
DOI: | 10.1016/j.physleta.2020.126570 |