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Fractional Solitons in Excitonic Josephson Junctions

dc.citation.epage0en_US
dc.citation.spage0en_US
dc.citation.volume5en_US
dc.citation.woscount3en_US
dc.contributor.authorHsu, Ya-Fenen_US
dc.contributor.authorSu, Jung-Jungen_US
dc.contributor.department電子物理學系zh_TW
dc.contributor.departmentDepartment of Electrophysicsen_US
dc.date.accessioned2019-04-03T06:36:22Z
dc.date.available2019-04-03T06:36:22Z
dc.date.issued2015-10-29en_US
dc.description.abstractThe Josephson effect is especially appealing to physicists because it reveals macroscopically the quantum order and phase. In excitonic bilayers the effect is even subtler due to the counterflow of supercurrent as well as the tunneling between layers (interlayer tunneling). Here we study, in a quantum Hall bilayer, the excitonic Josephson junction: a conjunct of two exciton condensates with a relative phase phi(0) applied. The system is mapped into a pseudospin ferromagnet then described numerically by the Landau-Lifshitz-Gilbert equation. In the presence of interlayer tunneling, we identify a family of fractional sine-Gordon solitons which resemble the static fractional Josephson vortices in the extended superconducting Josephson junctions. Each fractional soliton carries a topological charge Q that is not necessarily a half/full integer but can vary continuously. The calculated current-phase relation (CPR) shows that solitons with Q = phi(0)/2 pi is the lowest energy state starting from zero phi(0) - until phi(0) > pi - then the alternative group of solitons with Q = phi(0)/2 pi - 1 takes place and switches the polarity of CPR.en_US
dc.identifier.doi10.1038/srep15796en_US
dc.identifier.issn2045-2322en_US
dc.identifier.journalSCIENTIFIC REPORTSen_US
dc.identifier.urihttp://dx.doi.org/10.1038/srep15796en_US
dc.identifier.urihttps://ir.lib.nycu.edu.tw/handle/11536/128402
dc.identifier.wosnumberWOS:000363624200001en_US
dc.language.isoen_USen_US
dc.titleFractional Solitons in Excitonic Josephson Junctionsen_US
dc.typeArticleen_US

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