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dc.contributor.authorLu, Yao
dc.contributor.authorVirtanen, P.
dc.contributor.authorHeikkilä, Tero T.
dc.date.accessioned2022-08-24T11:11:35Z
dc.date.available2022-08-24T11:11:35Z
dc.date.issued2022
dc.identifier.citationLu, Y., Virtanen, P., & Heikkilä, T. T. (2022). Directly probing the chirality of Majorana edge states. <i>Physical Review B</i>, <i>106</i>(4), Article 045139. <a href="https://doi.org/10.1103/PhysRevB.106.045139" target="_blank">https://doi.org/10.1103/PhysRevB.106.045139</a>
dc.identifier.otherCONVID_151776795
dc.identifier.urihttps://jyx.jyu.fi/handle/123456789/82780
dc.description.abstractWe propose to directly probe the chirality of Majorana edge states in 2D topological superconductors using polarization selective photon absorption. When shining circularly polarized light on a 2D topological superconductor in disk geometry, the photons can excite quasiparticles only when the polarization of the light matches the chirality of the Majorana edge states required by the angular momentum conservation. Hence, one can obtain the chirality of the Majorana edge states by measuring the photon absorption rate. We show that the polarization selective photon absorption can also serve as smoking gun evidence of the chiral Majorana edge mode.en
dc.format.mimetypeapplication/pdf
dc.language.isoeng
dc.publisherAmerican Physical Society (APS)
dc.relation.ispartofseriesPhysical Review B
dc.rightsIn Copyright
dc.titleDirectly probing the chirality of Majorana edge states
dc.typeresearch article
dc.identifier.urnURN:NBN:fi:jyu-202208244314
dc.contributor.laitosFysiikan laitosfi
dc.contributor.laitosDepartment of Physicsen
dc.contributor.oppiaineNanoscience Centerfi
dc.contributor.oppiaineNanoscience Centeren
dc.type.urihttp://purl.org/eprint/type/JournalArticle
dc.type.coarhttp://purl.org/coar/resource_type/c_2df8fbb1
dc.description.reviewstatuspeerReviewed
dc.relation.issn2469-9950
dc.relation.numberinseries4
dc.relation.volume106
dc.type.versionpublishedVersion
dc.rights.copyright© 2022 American Physical Society
dc.rights.accesslevelopenAccessfi
dc.type.publicationarticle
dc.relation.grantnumber317118
dc.relation.grantnumber800923
dc.relation.grantnumber800923
dc.relation.projectidinfo:eu-repo/grantAgreement/EC/H2020/800923/EU//SUPERTED
dc.subject.ysofotonit
dc.subject.ysokvasihiukkaset
dc.subject.ysosuprajohteet
dc.format.contentfulltext
jyx.subject.urihttp://www.yso.fi/onto/yso/p2063
jyx.subject.urihttp://www.yso.fi/onto/yso/p38699
jyx.subject.urihttp://www.yso.fi/onto/yso/p9946
dc.rights.urlhttp://rightsstatements.org/page/InC/1.0/?language=en
dc.relation.doi10.1103/PhysRevB.106.045139
dc.relation.funderResearch Council of Finlanden
dc.relation.funderEuropean Commissionen
dc.relation.funderSuomen Akatemiafi
dc.relation.funderEuroopan komissiofi
jyx.fundingprogramAcademy Project, AoFen
jyx.fundingprogramFET Future and Emerging Technologies, H2020en
jyx.fundingprogramAkatemiahanke, SAfi
jyx.fundingprogramFET Future and Emerging Technologies, H2020fi
jyx.fundinginformationThis work was supported by the Academy of Finland (Project No. 317118). It has also received funding from the European Union's Horizon research and innovation programme under Grant Agreement No. 800923. We acknowledge grant PID2020-114252GB-I00 (SPIRIT) funded by MCIN/AEI/10.13039/501100011033 and by “ERDF A way of making Europe”. This work is funded by the Education Department of the Basque Government via the IKUR strategy program. 20-114252GB-I00 (SPIRIT).
dc.type.okmA1


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