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dc.contributor.authorKang, J. -H.en
dc.contributor.authorJung, S. -G.en
dc.contributor.authorLee, S.en
dc.contributor.authorPark, E.en
dc.contributor.authorLin, J. -Y.en
dc.contributor.authorChareev, D. A.en
dc.contributor.authorVasiliev, A. N.en
dc.contributor.authorPark, T.en
dc.date.accessioned2021-08-31T15:02:56Z-
dc.date.available2021-08-31T15:02:56Z-
dc.date.issued2016-
dc.identifier.citationPressure dependence of upper critical fields in FeSe single crystals / J. -H. Kang, S. -G. Jung, S. Lee, et al. — DOI 10.1088/0953-2048/29/3/035007 // Superconductor Science and Technology. — 2016. — Vol. 29. — Iss. 3. — 035007.en
dc.identifier.issn9532048-
dc.identifier.otherFinal2
dc.identifier.otherAll Open Access, Green3
dc.identifier.otherhttps://www.scopus.com/inward/record.uri?eid=2-s2.0-84960172257&doi=10.1088%2f0953-2048%2f29%2f3%2f035007&partnerID=40&md5=ea346a7485349e97b5b2499164a1dd2a
dc.identifier.otherhttp://arxiv.org/pdf/1602.03948m
dc.identifier.urihttp://elar.urfu.ru/handle/10995/102278-
dc.description.abstractWe investigate the pressure dependence of the upper critical fields (μ 0 H c2) for FeSe single crystals with pressure up to 2.57 GPa. The superconducting (SC) properties show a disparate behavior across a critical pressure where the pressure-induced antiferromagnetic phase coexists with superconductivity. The magnetoresistance for H//ab and H//c is very different: for H//c, magnetic field induces and enhances a hump in the resistivity close to the T c for pressures higher than 1.2 GPa, while it is absent for H//ab. Since the measured μ 0 H c2 for FeSe samples is smaller than the orbital limited upper critical field estimated by the Werthamer, Helfand and Hohenberg model, the Maki parameter (α) related to Pauli spin-paramagnetic effects is additionally considered to describe the temperature dependence of μ 0 H c2(T). Interestingly, the α value is hardly affected by pressure for H//ab, while it strongly increases with pressure for H//c. The pressure evolution of the μ 0 H c2(0) for the FeSe single crystals is found to be almost similar to that of T c(P), suggesting that the pressure-induced magnetic order adversely affects the upper critical fields as well as the SC transition temperature. © 2016 IOP Publishing Ltd.en
dc.format.mimetypeapplication/pdfen
dc.language.isoenen
dc.publisherInstitute of Physics Publishingen
dc.rightsinfo:eu-repo/semantics/openAccessen
dc.sourceSupercond Sci Technol2
dc.sourceSuperconductor Science and Technologyen
dc.subjectFESEen
dc.subjectMAKI PARAMETERen
dc.subjectPRESSUREen
dc.subjectUPPER CRITICAL FIELDen
dc.subjectENHANCED MAGNETORESISTANCEen
dc.subjectPRESSUREen
dc.subjectTEMPERATURE DISTRIBUTIONen
dc.subjectANTIFERROMAGNETIC PHASEen
dc.subjectFESEen
dc.subjectMAKI PARAMETERen
dc.subjectPARAMAGNETIC EFFECTen
dc.subjectPRESSURE DEPENDENCEen
dc.subjectPRESSURE-INDUCED MAGNETIC ORDERen
dc.subjectTEMPERATURE DEPENDENCEen
dc.subjectUPPER CRITICAL FIELDSen
dc.subjectSINGLE CRYSTALSen
dc.titlePressure dependence of upper critical fields in FeSe single crystalsen
dc.typeArticleen
dc.typeinfo:eu-repo/semantics/articleen
dc.typeinfo:eu-repo/semantics/publishedVersionen
dc.identifier.doi10.1088/0953-2048/29/3/035007-
dc.identifier.scopus84960172257-
local.contributor.employeeKang, J.-H., Department of Physics, Sungkyunkwan University, Suwon, 440-746, South Korea
local.contributor.employeeJung, S.-G., Department of Physics, Sungkyunkwan University, Suwon, 440-746, South Korea
local.contributor.employeeLee, S., Department of Physics, Sungkyunkwan University, Suwon, 440-746, South Korea
local.contributor.employeePark, E., Department of Physics, Sungkyunkwan University, Suwon, 440-746, South Korea
local.contributor.employeeLin, J.-Y., Institute of Physics, National Chiao Tung University, Hsinchu, 30010, Taiwan
local.contributor.employeeChareev, D.A., Institute of Experimental Mineralogy, Russian Academy of Sciences, Chernogolovka, Moscow Region, 142432, Russian Federation, Institute of Physics and Technology, Ural Federal University, Mira st. 19, Ekaterinburg, 620002, Russian Federation
local.contributor.employeeVasiliev, A.N., Low Temperature Physics and Superconductivity Department, Physics Faculty, Moscow State University, Moscow, 119991, Russian Federation, Theoretical Physics and Applied Mathematics Department, Institute of Physics and Technology, Ural Federal University, Ekaterinburg, 620002, Russian Federation, National University of Science and Technology 'Misis', Moscow, 119049, Russian Federation
local.contributor.employeePark, T., Department of Physics, Sungkyunkwan University, Suwon, 440-746, South Korea
local.issue3-
local.volume29-
local.contributor.departmentDepartment of Physics, Sungkyunkwan University, Suwon, 440-746, South Korea
local.contributor.departmentInstitute of Physics, National Chiao Tung University, Hsinchu, 30010, Taiwan
local.contributor.departmentInstitute of Experimental Mineralogy, Russian Academy of Sciences, Chernogolovka, Moscow Region, 142432, Russian Federation
local.contributor.departmentInstitute of Physics and Technology, Ural Federal University, Mira st. 19, Ekaterinburg, 620002, Russian Federation
local.contributor.departmentLow Temperature Physics and Superconductivity Department, Physics Faculty, Moscow State University, Moscow, 119991, Russian Federation
local.contributor.departmentTheoretical Physics and Applied Mathematics Department, Institute of Physics and Technology, Ural Federal University, Ekaterinburg, 620002, Russian Federation
local.contributor.departmentNational University of Science and Technology 'Misis', Moscow, 119049, Russian Federation
local.identifier.pure703467-
local.identifier.purec9dd2ab1-8cb0-4707-9e38-3e99711c53dbuuid
local.description.order035007-
local.identifier.eid2-s2.0-84960172257-
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