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dc.contributor.authorDomozhirova, A. N.en
dc.contributor.authorNaumov, S. V.en
dc.contributor.authorPodgornykh, S. M.en
dc.contributor.authorMarchenkova, E. B.en
dc.contributor.authorChistyakov, V. V.en
dc.contributor.authorHuang, J. C. A.en
dc.contributor.authorMarchenkov, V. V.en
dc.date.accessioned2021-08-31T15:08:00Z-
dc.date.available2021-08-31T15:08:00Z-
dc.date.issued2021-
dc.identifier.citationPeculiarities of the electro- And magnetoresistivity of WTe2and MoTe2single crystals before and after quenching / A. N. Domozhirova, S. V. Naumov, S. M. Podgornykh, et al. — DOI 10.1063/9.0000182 // AIP Advances. — 2021. — Vol. 11. — Iss. 1. — 015226.en
dc.identifier.issn21583226-
dc.identifier.otherFinal2
dc.identifier.otherAll Open Access, Gold3
dc.identifier.otherhttps://www.scopus.com/inward/record.uri?eid=2-s2.0-85099332997&doi=10.1063%2f9.0000182&partnerID=40&md5=63d843ed743a711f23b087766b1448e6
dc.identifier.otherhttps://aip.scitation.org/doi/pdf/10.1063/9.0000182m
dc.identifier.urihttp://elar.urfu.ru/handle/10995/103166-
dc.description.abstractWTe2 and MoTe2 single crystals were grown, some of them were quenched, and the following properties were studied: electroresistivity in the temperature range from 1.8 to 300 K, magnetoresistivity at temperatures from 1.8 to 300 K in magnetic fields of up to 9 T. On the one hand, quenching leads to dramatic changes in the behaviour and value of the electroresistivity of MoTe2; the type of the electroresistivity changes from "semiconductor"to "metallic", and the electroresistivity values of MoTe2 before and after quenching differ by 8 orders of magnitude (!) at low temperatures. On the other hand, quenching is shown not to lead to significant changes in the behaviour and value of the electroresistivity of WTe2. A relatively small increase in the electroresistivity of quenched WTe2 at low temperatures can be associated with the scattering of current carriers by structural defects. The magnetoresistivity of MoTe2 increases from 7 to 16% in a field of 9 T at a temperature of 12 K as a result of quenching. The magnetoresistivity of WTe2 is shown to reach ∼1700% in a field of 9 T at 2 K. The behaviour of the magnetoresistivity of non-quenched samples is typical for compensated conductors with a closed Fermi surface. © 2021 Author(s).en
dc.description.sponsorshipThe research was carried out within the state assignment of Ministry of Education and Science of the Russian Federation (theme “Spin”, No. AAAA-A18-118020290104-2), supported in part by RFBR (Project No. 20-32-90069) and the Government of the Russian Federation (Decree No. 211, Contract No. 02.A03.21.0006).en
dc.format.mimetypeapplication/pdfen
dc.language.isoenen
dc.publisherAmerican Institute of Physics Inc.en
dc.rightsinfo:eu-repo/semantics/openAccessen
dc.sourceAIP Adv.2
dc.sourceAIP Advancesen
dc.subjectMOLYBDENUM COMPOUNDSen
dc.subjectQUENCHINGen
dc.subjectTELLURIUM COMPOUNDSen
dc.subjectCURRENT CARRIERSen
dc.subjectLOW TEMPERATURESen
dc.subjectORDERS OF MAGNITUDEen
dc.subjectSTRUCTURAL DEFECTen
dc.subjectTEMPERATURE RANGEen
dc.subjectTUNGSTEN COMPOUNDSen
dc.titlePeculiarities of the electro- And magnetoresistivity of WTe2and MoTe2single crystals before and after quenchingen
dc.typeArticleen
dc.typeinfo:eu-repo/semantics/articleen
dc.typeinfo:eu-repo/semantics/publishedVersionen
dc.identifier.rsi45007435-
dc.identifier.doi10.1063/9.0000182-
dc.identifier.scopus85099332997-
local.contributor.employeeDomozhirova, A.N., M.N. Mikheev Institute of Metal Physics, Ub Ras, Ekaterinburg, 620108, Russian Federation
local.contributor.employeeNaumov, S.V., M.N. Mikheev Institute of Metal Physics, Ub Ras, Ekaterinburg, 620108, Russian Federation
local.contributor.employeePodgornykh, S.M., M.N. Mikheev Institute of Metal Physics, Ub Ras, Ekaterinburg, 620108, Russian Federation
local.contributor.employeeMarchenkova, E.B., M.N. Mikheev Institute of Metal Physics, Ub Ras, Ekaterinburg, 620108, Russian Federation
local.contributor.employeeChistyakov, V.V., M.N. Mikheev Institute of Metal Physics, Ub Ras, Ekaterinburg, 620108, Russian Federation
local.contributor.employeeHuang, J.C.A., National Cheng Kung University, Tainan, 70101, Taiwan
local.contributor.employeeMarchenkov, V.V., M.N. Mikheev Institute of Metal Physics, Ub Ras, Ekaterinburg, 620108, Russian Federation, Ural Federal University, Ekaterinburg, 620002, Russian Federation
local.issue1-
local.volume11-
dc.identifier.wos000609445800003-
local.contributor.departmentM.N. Mikheev Institute of Metal Physics, Ub Ras, Ekaterinburg, 620108, Russian Federation
local.contributor.departmentNational Cheng Kung University, Tainan, 70101, Taiwan
local.contributor.departmentUral Federal University, Ekaterinburg, 620002, Russian Federation
local.identifier.pure20518536-
local.identifier.pure6cf9ffbc-762c-4f6b-86fe-d4c144dbc592uuid
local.description.order015226-
local.identifier.eid2-s2.0-85099332997-
local.fund.rffi20-32-90069-
local.identifier.wosWOS:000609445800003-
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