Reexamining circular dichroism in photoemission from a topological insulator

dc.contributor.authorSidilkover, Ittai
dc.contributor.authorYen, Yun
dc.contributor.authorDsouza, Sunil Wilfred
dc.contributor.authorSchusser, Jakub
dc.contributor.authorPulkkinen, Aki Ismo Olavi
dc.contributor.authorRotundu, Costel R.
dc.contributor.authorHashimoto, Makoto
dc.contributor.authorLiu, Donghui
dc.contributor.authorShen, Zhi-Xun
dc.contributor.authorMinár, Jan
dc.contributor.authorSchüler, Michael
dc.contributor.authorSoifer, Hadas
dc.contributor.authorSobota, Jonathan A.
dc.date.accessioned2025-11-01T07:08:52Z
dc.date.available2025-11-01T07:08:52Z
dc.date.issued2025
dc.date.updated2025-11-01T07:08:52Z
dc.description.abstractThe orbital angular momentum (OAM) of electron states is an essential ingredient for topological and quantum geometric quantities in solids. For example, Dirac surface states with helical spin- and orbital-angular momenta are a hallmark of a 3D topological insulator. Angle-resolved photoemission spectroscopy (ARPES) with variable circular light polarization, known as circular dichroism (CD), has been assumed to be a direct probe of OAM and, by proxy, of the Berry curvature of electronic bands in energy- and momentum-space. Indeed, topological surface states have been shown to exhibit angle-dependent CD (CDAD), and more broadly, CD is often interpreted as evidence of spin-orbit coupling. Meanwhile, it is well-established that CD originates from the photoemission matrix elements, which can have extrinsic contributions related to the experimental geometry and the inherently broken inversion symmetry at the sample surface. Therefore, it is important to broadly examine CD-ARPES to determine the scenarios in which it provides a robust probe of intrinsic material physics. We performed CDARPES on the canonical topological insulator Bi2Se3 over a wide range of incident photon energies. Not only do we observe angle-dependent CD in the surface states, as expected, but we also find CD of a similar magnitude in virtually all bulk bands. Since OAM is forbidden by inversion symmetry in the bulk, we conclude this originates from symmetry-breaking in the photoemission process. Comparison with theoretical calculations supports this view and suggests that "hidden" OAM-localized to atomic sites within each unit cell-contributes significantly. Additional effects, including inter-atomic interference and final-state resonances, are responsible for the rapid variation of the CDAD signal with photon energy.en
dc.format14
dc.identifier.document-number001528356400017
dc.identifier.doi10.1103/g9d4-qls9
dc.identifier.issn2643-1564
dc.identifier.obd43947452
dc.identifier.orcidDsouza, Sunil Wilfred 0000-0001-5889-3399
dc.identifier.orcidSchusser, Jakub 0000-0001-8260-0234
dc.identifier.orcidPulkkinen, Aki Ismo Olavi 0000-0002-4339-6928
dc.identifier.orcidMinár, Jan 0000-0001-9735-8479
dc.identifier.urihttp://hdl.handle.net/11025/63381
dc.language.isoen
dc.project.IDEH22_008/0004572
dc.relation.ispartofseriesPhysical Review Research
dc.rights.accessA
dc.subjectweyl semimetal phaseen
dc.subjectlighten
dc.titleReexamining circular dichroism in photoemission from a topological insulatoren
dc.typeČlánek v databázi WoS (Jimp)
dc.typeČLÁNEK
dc.type.statusPublished Version
local.files.count1*
local.files.size6584697*
local.has.filesyes*

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