Microwave-induced transitions between weak localization and weak antilocalization in graphene

dc.contributor.authorNavarro Giraldo, Jorge Andrescs
dc.contributor.authorSantana, Vinicius Tadeucs
dc.contributor.authorLaguta, Oleksiics
dc.contributor.authorBloos, Dominikcs
dc.contributor.authorBauernfeind, Anastasiacs
dc.contributor.authorScheffler, Marccs
dc.contributor.authorLaguta, Valentyncs
dc.contributor.authorGaskill, D. Kurtcs
dc.contributor.authorNeugebauer, Petrcs
dc.coverage.issueMarchcs
dc.coverage.volume113cs
dc.date.accessioned2026-03-16T10:54:04Z
dc.date.issued2026-03-04cs
dc.description.abstractWeak localization (WL) and weak antilocalization (WAL) of electrons in a disordered conductor refer to the decrease or increase of the conductivity caused by the quantum interference of the electronic motion. In graphene, the nontrivial Berry phase and the chiral nature of the charge carriers imply that both phenomena can be observed, as it has been firmly established in direct current (DC) magnetotransport experiments. However, studies of alternating current (AC) magnetoconductivity at frequencies comparable to, and much higher than, the dephasing rate (1) remain unexplored. Using a combination of transport and spectroscopic measurements at low (/2en
dc.formattextcs
dc.format.extent1-13cs
dc.format.mimetypeapplication/pdfcs
dc.identifier.citationPhysical Review B. 2026, vol. 113, issue March, p. 1-13.en
dc.identifier.doi10.1103/8nz6-xgg5cs
dc.identifier.issn2469-9950cs
dc.identifier.orcid0000-0003-1440-4703cs
dc.identifier.orcid0000-0002-2258-6140cs
dc.identifier.orcid0000-0002-3567-414Xcs
dc.identifier.orcid0000-0001-9421-4349cs
dc.identifier.orcid0009-0002-3710-5722cs
dc.identifier.orcid0000-0002-7044-7532cs
dc.identifier.orcid0000-0003-3072-247Xcs
dc.identifier.orcid0000-0001-7106-3605cs
dc.identifier.orcid0000-0001-7095-6401cs
dc.identifier.other201712cs
dc.identifier.researcheridJWA-1451-2024cs
dc.identifier.researcheridB-5381-2014cs
dc.identifier.researcheridF-4961-2019cs
dc.identifier.researcheridI-7844-2013cs
dc.identifier.scopus57202677107cs
dc.identifier.scopus54788236000cs
dc.identifier.urihttps://hdl.handle.net/11012/256423
dc.language.isoencs
dc.publisherAmerican Physical Societycs
dc.relation.ispartofPhysical Review Bcs
dc.relation.urihttps://journals.aps.org/prb/abstract/10.1103/8nz6-xgg5cs
dc.rightsCreative Commons Attribution 4.0 Internationalcs
dc.rights.accessopenAccesscs
dc.rights.sherpahttp://www.sherpa.ac.uk/romeo/issn/2469-9950/cs
dc.rights.urihttp://creativecommons.org/licenses/by/4.0/cs
dc.subjectOptical & microwave phenomenaen
dc.subjectMagneto-opticsen
dc.subjectMagnetotransporten
dc.subjectWeak antilocalizationen
dc.subjectWeak localizationen
dc.titleMicrowave-induced transitions between weak localization and weak antilocalization in grapheneen
dc.type.driverarticleen
dc.type.statusPeer-revieweden
dc.type.versionpublishedVersionen
eprints.grantNumberinfo:eu-repo/grantAgreement/GA0/GA/GA23-05578Scs
sync.item.dbidVAV-201712en
sync.item.dbtypeVAVen
sync.item.insts2026.03.16 11:54:04en
sync.item.modts2026.03.16 11:33:46en
thesis.grantorVysoké učení technické v Brně. Středoevropský technologický institut VUT. Magneto-Optická a THz Spektroskopiecs
thesis.grantorVysoké učení technické v Brně. Středoevropský technologický institut VUT. Kvantový molekulární magnetismuscs

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