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dc.contributor.authorMinkov, G. M.en
dc.contributor.authorAleshkin, V. Y.en
dc.contributor.authorRut, O. E.en
dc.contributor.authorSherstobitov, A. A.en
dc.contributor.authorGermanenko, A. V.en
dc.contributor.authorDvoretski, S. A.en
dc.contributor.authorMikhailov, N. N.en
dc.date.accessioned2021-08-31T15:00:00Z-
dc.date.available2021-08-31T15:00:00Z-
dc.date.issued2019-
dc.identifier.citationSpin-orbit splitting of the conduction band in HgTe quantum wells: Role of different mechanisms / G. M. Minkov, V. Y. Aleshkin, O. E. Rut, et al. — DOI 10.1016/j.physe.2019.02.007 // Physica E: Low-Dimensional Systems and Nanostructures. — 2019. — Vol. 110. — P. 95-99.en
dc.identifier.issn13869477-
dc.identifier.otherFinal2
dc.identifier.otherAll Open Access, Green3
dc.identifier.otherhttps://www.scopus.com/inward/record.uri?eid=2-s2.0-85061823066&doi=10.1016%2fj.physe.2019.02.007&partnerID=40&md5=911edb3fb9c4f48fb715b5cc50e7113d
dc.identifier.otherhttp://arxiv.org/pdf/1807.03598m
dc.identifier.urihttp://elar.urfu.ru/handle/10995/101814-
dc.description.abstractSpin-orbit splitting of conduction band in HgTe quantum wells was studied experimentally. In order to recognize the role of different mechanisms, we carried out detailed measurements of the Shubnikov-de Haas oscillations in gated structures with a quantum well widths from 8 to 18 nm over a wide range of electron density. With increasing electron density controlled by the gate voltage, splitting of the maximum of the oscillation Fourier spectrum f 0 into two components f 1 and f 2 and the appearance of the low-frequency component f 3 was observed. Our analysis shows that the components f 1 and f 2 are determined by the electron densities n 1 and n 2 in spin-orbit split subbands while the f 3 component results from magneto-intersubband oscillations so that it is determined by the difference between these densities Δn. This allows us to obtain all three values n 1 , n 2 and Δn independently. Comparison of the data obtained with results of self-consistent calculations carried out within the framework of four-band kP model shows that the main contribution to spin-orbit splitting comes from the Bychkov-Rashba effect. Contribution of the interface inversion asymmetry to the splitting of the conduction band turns out to be four-to-five times less than that for the valence band in the same structures. © 2019 Elsevier B.V.en
dc.format.mimetypeapplication/pdfen
dc.language.isoenen
dc.publisherElsevier B.V.en
dc.rightsinfo:eu-repo/semantics/openAccessen
dc.sourcePhys E2
dc.sourcePhysica E: Low-Dimensional Systems and Nanostructuresen
dc.subjectELECTRON TRANSPORTen
dc.subjectENERGY SPECTRUMen
dc.subjectQUANTUM WELLSen
dc.subjectCARRIER CONCENTRATIONen
dc.subjectCONDUCTION BANDSen
dc.subjectELECTRON DENSITY MEASUREMENTen
dc.subjectELECTRON TRANSPORT PROPERTIESen
dc.subjectMERCURY COMPOUNDSen
dc.subjectQUANTUM CHEMISTRYen
dc.subjectTELLURIUM COMPOUNDSen
dc.subjectDIFFERENT MECHANISMSen
dc.subjectELECTRON TRANSPORTen
dc.subjectENERGY SPECTRAen
dc.subjectINVERSION ASYMMETRYen
dc.subjectLOW-FREQUENCY COMPONENTSen
dc.subjectSELF-CONSISTENT CALCULATIONen
dc.subjectSHUBNIKOV DE-HAAS OSCILLATIONen
dc.subjectSPIN-ORBIT SPLITTINGSen
dc.subjectSEMICONDUCTOR QUANTUM WELLSen
dc.titleSpin-orbit splitting of the conduction band in HgTe quantum wells: Role of different mechanismsen
dc.typeArticleen
dc.typeinfo:eu-repo/semantics/articleen
dc.typeinfo:eu-repo/semantics/publishedVersionen
dc.identifier.doi10.1016/j.physe.2019.02.007-
dc.identifier.scopus85061823066-
local.contributor.employeeMinkov, G.M., School of Natural Sciences and Mathematics, Ural Federal University, Ekaterinburg, 620002, Russian Federation
local.contributor.employeeAleshkin, V.Y., Institute for Physics of Microstructures RAS, Nizhny Novgorod, 603950, Russian Federation
local.contributor.employeeRut, O.E., School of Natural Sciences and Mathematics, Ural Federal University, Ekaterinburg, 620002, Russian Federation
local.contributor.employeeSherstobitov, A.A., School of Natural Sciences and Mathematics, Ural Federal University, Ekaterinburg, 620002, Russian Federation, M.N. Mikheev Institute of Metal Physics of the Ural Branch of the Russian Academy of Sciences, Ekaterinburg, 620108, Russian Federation
local.contributor.employeeGermanenko, A.V., School of Natural Sciences and Mathematics, Ural Federal University, Ekaterinburg, 620002, Russian Federation
local.contributor.employeeDvoretski, S.A., Institute of Semiconductor Physics RAS, Novosibirsk, 630090, Russian Federation
local.contributor.employeeMikhailov, N.N., Institute of Semiconductor Physics RAS, Novosibirsk, 630090, Russian Federation, Novosibirsk State University, Novosibirsk, 630090, Russian Federation
local.description.firstpage95-
local.description.lastpage99-
local.volume110-
dc.identifier.wos000460542000016-
local.contributor.departmentSchool of Natural Sciences and Mathematics, Ural Federal University, Ekaterinburg, 620002, Russian Federation
local.contributor.departmentInstitute for Physics of Microstructures RAS, Nizhny Novgorod, 603950, Russian Federation
local.contributor.departmentM.N. Mikheev Institute of Metal Physics of the Ural Branch of the Russian Academy of Sciences, Ekaterinburg, 620108, Russian Federation
local.contributor.departmentInstitute of Semiconductor Physics RAS, Novosibirsk, 630090, Russian Federation
local.contributor.departmentNovosibirsk State University, Novosibirsk, 630090, Russian Federation
local.identifier.pure4c86739d-7b13-4a4c-ba6a-facd29f4f45fuuid
local.identifier.pure9056104-
local.identifier.eid2-s2.0-85061823066-
local.identifier.wosWOS:000460542000016-
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