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dc.contributor.authorMorozova, N. V.en
dc.contributor.authorKorobeinikov, I. V.en
dc.contributor.authorKurochka, K. V.en
dc.contributor.authorOvsyannikov, S. V.en
dc.date.accessioned2021-08-31T15:06:28Z-
dc.date.available2021-08-31T15:06:28Z-
dc.date.issued2020-
dc.identifier.citationColossal variations in the thermopower and n-p conductivity switching in topological tellurides under pressure / N. V. Morozova, I. V. Korobeinikov, K. V. Kurochka, et al. — DOI 10.1063/5.0031818 // Journal of Applied Physics. — 2020. — Vol. 128. — Iss. 24. — 245902.en
dc.identifier.issn218979-
dc.identifier.otherFinal2
dc.identifier.otherAll Open Access, Bronze3
dc.identifier.otherhttps://www.scopus.com/inward/record.uri?eid=2-s2.0-85099204151&doi=10.1063%2f5.0031818&partnerID=40&md5=a24d17b9fe748cc9a15816a7549ab571
dc.identifier.urihttp://elar.urfu.ru/handle/10995/102937-
dc.description.abstractUnder applied high pressure, the electronic, optical, structural, and other properties of narrow-bandgap telluride semiconductors are subjected to dramatic changes. They can include, for instance, structural and electronic topological transitions. In this work, we investigated the electronic properties of single crystals of three families of tellurides, namely, HgTe, PbTe, and Bi2Te3 by measurements of the thermoelectric power (the Seebeck coefficient) and electrical resistance under high pressure up to 10 GPa. The applied pressure led to spectacular variations in the electronic transport of all three tellurides. We addressed these effects to electronic topological transitions that could be driven by significant narrowing of the bandgaps in the normal-pressure phases of these compounds. In particular, at about 1 GPa, we observed an n-p switching in the conductivity of HgTe, which was well reproducible under multiple pressure cycling. In contrast, in PbTe, we found that an electronic topological transition irreversibly turns the conductivity from p- to n-type. An electronic topological Lifshitz transition in p-type Bi2Te3 crystals with a low carrier concentration enhanced the n-type conductivity in a narrow pressure region about 2-3 GPa and resulted in a double p-n-p conductivity inversion. An irreversible p-n conductivity switching in p-type Bi2Te3 happened already on decompression from a high-pressure phase from about 8 GPa. The stress-controlled p-n inversions of the electrical conductivity in these industrially important telluride materials can potentially find emergent applications in micro- and nanoelectronics. © 2020 Author(s).en
dc.description.sponsorshipThe research was supported by a grant of Ministry of Science and Higher Education of the Russian Federation No. 075-15-2020-797 (13.1902.21.0024).en
dc.format.mimetypeapplication/pdfen
dc.language.isoenen
dc.publisherAmerican Institute of Physics Inc.en
dc.rightsinfo:eu-repo/semantics/openAccessen
dc.sourceJ Appl Phys2
dc.sourceJournal of Applied Physicsen
dc.subjectBISMUTH COMPOUNDSen
dc.subjectCARRIER CONCENTRATIONen
dc.subjectELECTRONIC PROPERTIESen
dc.subjectENERGY GAPen
dc.subjectIV-VI SEMICONDUCTORSen
dc.subjectLEAD COMPOUNDSen
dc.subjectMERCURY COMPOUNDSen
dc.subjectNARROW BAND GAP SEMICONDUCTORSen
dc.subjectTHERMOELECTRIC POWER PLANTSen
dc.subjectTOPOLOGYen
dc.subjectCONDUCTIVITY SWITCHINGen
dc.subjectELECTRICAL CONDUCTIVITYen
dc.subjectELECTRICAL RESISTANCESen
dc.subjectELECTRONIC TOPOLOGICAL TRANSITIONen
dc.subjectELECTRONIC TRANSPORTen
dc.subjectHIGH-PRESSURE PHASEen
dc.subjectLIFSHITZ TRANSITIONen
dc.subjectN-TYPE CONDUCTIVITYen
dc.subjectTELLURIUM COMPOUNDSen
dc.titleColossal variations in the thermopower and n-p conductivity switching in topological tellurides under pressureen
dc.typeArticleen
dc.typeinfo:eu-repo/semantics/articleen
dc.typeinfo:eu-repo/semantics/publishedVersionen
dc.identifier.doi10.1063/5.0031818-
dc.identifier.scopus85099204151-
local.contributor.employeeMorozova, N.V., M. N. Miheev Institute of Metal Physics, Ural Branch of Russian Academy of Sciences, 18 S. Kovalevskaya Str., Yekaterinburg, 620137, Russian Federation
local.contributor.employeeKorobeinikov, I.V., M. N. Miheev Institute of Metal Physics, Ural Branch of Russian Academy of Sciences, 18 S. Kovalevskaya Str., Yekaterinburg, 620137, Russian Federation
local.contributor.employeeKurochka, K.V., M. N. Miheev Institute of Metal Physics, Ural Branch of Russian Academy of Sciences, 18 S. Kovalevskaya Str., Yekaterinburg, 620137, Russian Federation, Institute of Natural Sciences and Mathematics, Ural Federal University, 19 Mira St., Yekaterinburg, 620002, Russian Federation
local.contributor.employeeOvsyannikov, S.V., Bayerisches Geoinstitut, Universität Bayreuth, Universitätsstrasse 30, Bayreuth, D-95447, Germany, Institute for Solid State Chemistry, Ural Branch of Russian Academy of Sciences, 91 Pervomayskaya St., Yekaterinburg, 620219, Russian Federation
local.issue24-
local.volume128-
dc.identifier.wos000602993700002-
local.contributor.departmentM. N. Miheev Institute of Metal Physics, Ural Branch of Russian Academy of Sciences, 18 S. Kovalevskaya Str., Yekaterinburg, 620137, Russian Federation
local.contributor.departmentInstitute of Natural Sciences and Mathematics, Ural Federal University, 19 Mira St., Yekaterinburg, 620002, Russian Federation
local.contributor.departmentBayerisches Geoinstitut, Universität Bayreuth, Universitätsstrasse 30, Bayreuth, D-95447, Germany
local.contributor.departmentInstitute for Solid State Chemistry, Ural Branch of Russian Academy of Sciences, 91 Pervomayskaya St., Yekaterinburg, 620219, Russian Federation
local.identifier.puree4109a3c-6cc8-42a0-8886-aa793e41c0dduuid
local.identifier.pure20519818-
local.description.order245902-
local.identifier.eid2-s2.0-85099204151-
local.identifier.wosWOS:000602993700002-
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