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dc.contributor.authorTalantsev, E. F.en
dc.date.accessioned2021-08-31T14:59:12Z-
dc.date.available2021-08-31T14:59:12Z-
dc.date.issued2019-
dc.identifier.citationTalantsev E. F. Classifying hydrogen-rich superconductors / E. F. Talantsev. — DOI 10.1088/2053-1591/ab3bbb // Materials Research Express. — 2019. — Vol. 6. — Iss. 10. — 106002.en
dc.identifier.issn20531591-
dc.identifier.otherFinal2
dc.identifier.otherAll Open Access, Green3
dc.identifier.otherhttps://www.scopus.com/inward/record.uri?eid=2-s2.0-85071670041&doi=10.1088%2f2053-1591%2fab3bbb&partnerID=40&md5=9dc7e0b4889ba65423163a98a5388198
dc.identifier.otherhttp://arxiv.org/pdf/1906.07650m
dc.identifier.urihttp://elar.urfu.ru/handle/10995/101709-
dc.description.abstractThe era of near-room-temperature superconductivity started after experimental discovery by Drozdov et al (2015 Nature 525 73) who found that compressed H3S exhibits superconducting transition at T c = 203 K. To date, the record near-room-temperature superconductivity stands with another hydrogen-rich highly compressed compound, LaH10 (Somayazulu et al 2019 Phys. Rev. Lett. 122 027001), which has critical temperature of In this paper, we analyse available upper critical field, B c2(T), data for LaH10 (Drozdov et al 2019 Nature 569 528) and report that this compound in all considered scenarios has the ratio of T c to the Fermi temperature, T F, 0.009 < T c/T F < 0.038, which is typical range for unconventional superconductors. In attempt to extend our finding, we examined experimental B c2(T) data for superconductors in the palladium-hydrogen system and surprisingly find that PdHx compounds have the ratio of 0.008 < T c/T F < 0.012. Taking in account that H3S has the ratio of 0.012 < T c/T F < 0.039 (Talantsev 2019 Modern Phys. Lett. B 33 1950195) we come to conclusion that in the Uemura plot all discovered to date hydrogen-rich superconductors, i.e. PdHx, H3S and LaH10, lie in same band as all unconventional superconductors, particularly heavy fermions, fullerenes, pnictides, and cuprates, and former should be classified as a new class of unconventional superconductors. © 2019 IOP Publishing Ltd.en
dc.format.mimetypeapplication/pdfen
dc.language.isoenen
dc.publisherInstitute of Physics Publishingen
dc.rightsinfo:eu-repo/semantics/openAccessen
dc.sourceMater. Res. Express2
dc.sourceMaterials Research Expressen
dc.subjectHYDROGEN-RICH SUPERCONDUCTING COMPOUNDSen
dc.subjectLANTHANUM DECAHYDRIDEen
dc.subjectUNCONVENTIONAL SUPERCONDUCTIVITYen
dc.subjectUPPER CRITICAL FIELDen
dc.subjectCOPPER COMPOUNDSen
dc.subjectHEAVY FERMION SUPERCONDUCTORSen
dc.subjectPALLADIUM COMPOUNDSen
dc.subjectCRITICAL TEMPERATURESen
dc.subjectFERMI TEMPERATUREen
dc.subjectNEAR ROOM TEMPERATUREen
dc.subjectSUPERCONDUCTING COMPOUNDSen
dc.subjectSUPERCONDUCTING TRANSITIONSen
dc.subjectUNCONVENTIONAL SUPERCONDUCTIVITYen
dc.subjectUNCONVENTIONAL SUPERCONDUCTORSen
dc.subjectUPPER CRITICAL FIELDSen
dc.subjectLANTHANUM COMPOUNDSen
dc.titleClassifying hydrogen-rich superconductorsen
dc.typeArticleen
dc.typeinfo:eu-repo/semantics/articleen
dc.typeinfo:eu-repo/semantics/publishedVersionen
dc.identifier.doi10.1088/2053-1591/ab3bbb-
dc.identifier.scopus85071670041-
local.contributor.employeeTalantsev, E.F., M.N. Miheev Institute of Metal Physics, Ural Branch, Russian Academy of Sciences, S. Kovalevskoy St. 18, Ekaterinburg, 620108, Russian Federation, NANOTECH Centre, Ural Federal University, 19 Mira St., Ekaterinburg, 620002, Russian Federation
local.issue10-
local.volume6-
dc.identifier.wos000483109900002-
local.contributor.departmentM.N. Miheev Institute of Metal Physics, Ural Branch, Russian Academy of Sciences, S. Kovalevskoy St. 18, Ekaterinburg, 620108, Russian Federation
local.contributor.departmentNANOTECH Centre, Ural Federal University, 19 Mira St., Ekaterinburg, 620002, Russian Federation
local.identifier.pure32464cd5-e403-4d18-93cc-307178775471uuid
local.identifier.pure10774560-
local.description.order106002-
local.identifier.eid2-s2.0-85071670041-
local.identifier.wosWOS:000483109900002-
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