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dc.contributor.authorRosenstein, Baruchen_US
dc.contributor.authorShapiro, B. Ya.en_US
dc.contributor.authorLi, Dingpingen_US
dc.contributor.authorShapiro, I.en_US
dc.date.accessioned2019-04-03T06:41:33Z-
dc.date.available2019-04-03T06:41:33Z-
dc.date.issued2017-12-29en_US
dc.identifier.issn2469-9950en_US
dc.identifier.urihttp://dx.doi.org/10.1103/PhysRevB.96.224517en_US
dc.identifier.urihttp://hdl.handle.net/11536/144311-
dc.description.abstractMicroscopic theory of the normal-to-superconductor coexistence line of a multiband Weyl superconductor subjected to magnetic field is constructed. It is shown that the Weyl semimetal that is nonsuperconducting or having a small critical temperature T-c at zero field might become a superconductor at higher temperatures when the magnetic field is tuned to a series of quantized values H-n. The pairing occurs on Landau levels. It is argued that the phenomenon is detectable much easier in Weyl semimetals than in parabolic band metals since the quantum limit already has been approached in several Weyl materials. The effect of Zeeman coupling leading to splitting of the reentrant superconducting regions on the magnetic phase diagram is considered. An experimental signature of the superconductivity on Landau levels is the reduction of magnetoresistivity. This has been observed already in Cd3As2 and several other compounds. The novel kind of quantum oscillations of magnetoresistance detected in ZrTe5 is discussed along these lines.en_US
dc.language.isoen_USen_US
dc.titleStrong magnetic field induces superconductivity in a Weyl semimetalen_US
dc.typeArticleen_US
dc.identifier.doi10.1103/PhysRevB.96.224517en_US
dc.identifier.journalPHYSICAL REVIEW Ben_US
dc.citation.volume96en_US
dc.citation.issue22en_US
dc.citation.spage0en_US
dc.citation.epage0en_US
dc.contributor.department電子物理學系zh_TW
dc.contributor.departmentDepartment of Electrophysicsen_US
dc.identifier.wosnumberWOS:000419000900007en_US
dc.citation.woscount4en_US
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