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dc.contributor.authorCho, C. -W.en
dc.contributor.authorNg, C. Y.en
dc.contributor.authorWong, C. H.en
dc.contributor.authorAbdel-Hafiez, M.en
dc.contributor.authorVasiliev, A. N.en
dc.contributor.authorChareev, D. A.en
dc.contributor.authorLebed, A. G.en
dc.contributor.authorLortz, R.en
dc.date.accessioned2022-10-19T05:23:33Z-
dc.date.available2022-10-19T05:23:33Z-
dc.date.issued2022-
dc.identifier.citationCompetition between orbital effects, Pauli limiting, and Fulde-Ferrell-Larkin-Ovchinnikov states in 2D transition metal dichalcogenide superconductors / C. -W. Cho, C. Y. Ng, C. H. Wong et al. // New Journal of Physics. — 2022. — Vol. 24. — Iss. 8. — 83001.en
dc.identifier.issn13672630-
dc.identifier.otherhttps://www.scopus.com/inward/record.uri?eid=2-s2.0-85135984424&doi=10.1088%2f1367-2630%2fac8114&partnerID=40&md5=6e2f02e6d45834c02d4c989dc44115dclink
dc.identifier.urihttp://elar.urfu.ru/handle/10995/118199-
dc.description.abstractWe compare the upper critical field of bulk single-crystalline samples of the two intrinsic transition metal dichalcogenide superconductors, 2H-NbSe2 and 2H-NbS2, in high magnetic fields where their layer structure is aligned strictly parallel and perpendicular to the field, using magnetic torque experiments and a high-precision piezo-rotary positioner. While both superconductors show that orbital effects still have a significant impact when the layer structure is aligned parallel to the field, the upper critical field of NbS2 rises above the Pauli limiting field and forms a Fulde-Ferrell-Larkin-Ovchinnikov (FFLO) state, while orbital effects suppress superconductivity in NbSe2 just below the Pauli limit, which excludes the formation of the FFLO state. From the out-of-plane anisotropies, the coherence length perpendicular to the layers of 31 Å in NbSe2 is much larger than the interlayer distance, leading to a significant orbital effect suppressing superconductivity before the Pauli limit is reached, in contrast to the more 2D NbS2 © 2022 The Author(s). Published by IOP Publishing Ltd on behalf of the Institute of Physics and Deutsche Physikalische Gesellschaften
dc.description.sponsorship075-15-2021-604; Research Grants Council, University Grants Committee, 研究資助局: GRF-16302018, GRF-16303820, SBI17SC14; Vetenskapsrådet, VR: 2018-05393en
dc.description.sponsorshipWe thank U Lampe for technical assistance. This work was supported by Grants from the Research Grants Council of the Hong Kong Special Administrative Region, China (GRF-16302018, GRF-16303820, C6025-19G-A, SBI17SC14). MAH acknowledge the financial support from the Swedish Research Council (VR) under Project No. 2018-05393. Support by the P220 program of Government of Russia through the project 075-15-2021-604 is acknowledged.en
dc.format.mimetypeapplication/pdfen
dc.language.isoenen
dc.publisherInstitute of Physicsen
dc.rightsinfo:eu-repo/semantics/openAccessen
dc.sourceNew Journal of Physicsen
dc.subjectFULDE-FERRELL-LARKIN-OVCHINNIKOV STATEen
dc.subjectNBS2en
dc.subjectNBSE2en
dc.subjectSUPERCONDUCTIVITYen
dc.subjectTRANSITION METAL DICHALCOGENIDEen
dc.subjectSELENIUM COMPOUNDSen
dc.subjectSULFUR COMPOUNDSen
dc.subjectSUPERCONDUCTING MATERIALSen
dc.subjectTRANSITION METALSen
dc.subjectCRYSTALLINE SAMPLESen
dc.subjectFULDE-FERRELL-LARKIN-OVCHINNIKOV STATEen
dc.subjectINSTITUTE OF PHYSICSen
dc.subjectLAYER STRUCTURESen
dc.subjectORBITAL EFFECTSen
dc.subjectPAULI LIMITen
dc.subjectSINGLE-CRYSTALLINEen
dc.subjectTRANSITION METAL DICHALCOGENIDES (TMD)en
dc.subjectUPPER CRITICAL FIELDSen
dc.subjectUPPERCRITICAL FIELDSen
dc.subjectNIOBIUM COMPOUNDSen
dc.titleCompetition between orbital effects, Pauli limiting, and Fulde-Ferrell-Larkin-Ovchinnikov states in 2D transition metal dichalcogenide superconductorsen
dc.typeArticleen
dc.typeinfo:eu-repo/semantics/articleen
dc.typeinfo:eu-repo/semantics/publishedVersionen
dc.identifier.doi10.1088/1367-2630/ac8114-
dc.identifier.scopus85135984424-
local.contributor.employeeCho, C.-W., Department of Physics, The Hong Kong University of Science and Technology, Clear Water Bay, Kowloon, Hong Kongen
local.contributor.employeeNg, C.Y., Department of Physics, The Hong Kong University of Science and Technology, Clear Water Bay, Kowloon, Hong Kongen
local.contributor.employeeWong, C.H., Department of Industrial and Systems Engineering, The Hong Kong Polytechnic University, 11 Yuk Choi Rd, Hung Hom, Kowloon, Hong Kongen
local.contributor.employeeAbdel-Hafiez, M., Department of Physics and Astronomy, Uppsala University, Uppsala, SE-75120, Sweden, Lyman Laboratory of Physics, Harvard University, Cambridge, MA 02138, United Statesen
local.contributor.employeeVasiliev, A.N., Department of Low Temperature Physics and Superconductivity, Lomonosov Moscow State University, Moscow, 119991, Russian Federation, Quantum Functional Materials Laboratory, National University of Science and Technology ‘MISiS’, Moscow, 119049, Russian Federation, Ural Federal University, Ekaterinburg, 620002, Russian Federationen
local.contributor.employeeChareev, D.A., Quantum Functional Materials Laboratory, National University of Science and Technology ‘MISiS’, Moscow, 119049, Russian Federation, Ural Federal University, Ekaterinburg, 620002, Russian Federation, Institute of Experimental Mineralogy, RAS, Chernogolovka, Moscow Region, 142432, Russian Federationen
local.contributor.employeeLebed, A.G., Department of Physics, University of Arizona, 1118 E. 4th Street, Tucson, AZ 85721, United States, Landau Institute for Theoretical Physics, RAS, 2 Kosygina Street, Moscow, 117334, Russian Federationen
local.contributor.employeeLortz, R., Department of Physics, The Hong Kong University of Science and Technology, Clear Water Bay, Kowloon, Hong Kongen
local.issue8-
local.volume24-
dc.identifier.wos000840154800001-
local.contributor.departmentDepartment of Physics, The Hong Kong University of Science and Technology, Clear Water Bay, Kowloon, Hong Kongen
local.contributor.departmentDepartment of Industrial and Systems Engineering, The Hong Kong Polytechnic University, 11 Yuk Choi Rd, Hung Hom, Kowloon, Hong Kongen
local.contributor.departmentDepartment of Physics and Astronomy, Uppsala University, Uppsala, SE-75120, Swedenen
local.contributor.departmentLyman Laboratory of Physics, Harvard University, Cambridge, MA 02138, United Statesen
local.contributor.departmentDepartment of Low Temperature Physics and Superconductivity, Lomonosov Moscow State University, Moscow, 119991, Russian Federationen
local.contributor.departmentQuantum Functional Materials Laboratory, National University of Science and Technology ‘MISiS’, Moscow, 119049, Russian Federationen
local.contributor.departmentUral Federal University, Ekaterinburg, 620002, Russian Federationen
local.contributor.departmentInstitute of Experimental Mineralogy, RAS, Chernogolovka, Moscow Region, 142432, Russian Federationen
local.contributor.departmentDepartment of Physics, University of Arizona, 1118 E. 4th Street, Tucson, AZ 85721, United Statesen
local.contributor.departmentLandau Institute for Theoretical Physics, RAS, 2 Kosygina Street, Moscow, 117334, Russian Federationen
local.identifier.pure30749604-
local.description.order83001-
local.identifier.eid2-s2.0-85135984424-
local.identifier.wosWOS:000840154800001-
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