Please use this identifier to cite or link to this item: http://elar.urfu.ru/handle/10995/101415
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dc.contributor.authorTalantsev, E. F.en
dc.date.accessioned2021-08-31T14:57:05Z-
dc.date.available2021-08-31T14:57:05Z-
dc.date.issued2020-
dc.identifier.citationTalantsev E. F. Advanced McMillan's equation and its application for the analysis of highly-compressed superconductors / E. F. Talantsev. — DOI 10.1088/1361-6668/ab953f // Superconductor Science and Technology. — 2020. — Vol. 33. — Iss. 9. — 094009.en
dc.identifier.issn9532048-
dc.identifier.otherFinal2
dc.identifier.otherAll Open Access, Green3
dc.identifier.otherhttps://www.scopus.com/inward/record.uri?eid=2-s2.0-85091760337&doi=10.1088%2f1361-6668%2fab953f&partnerID=40&md5=2b193d0a9c1a6b05334c4a701fd063d7
dc.identifier.otherhttp://arxiv.org/pdf/2002.12859m
dc.identifier.urihttp://elar.urfu.ru/handle/10995/101415-
dc.description.abstractAny theory of electron-phonon mediated superconductivity requires knowledge of the full phonon spectrum α2 in order to calculate superconducting transition temperature, T c. However, there is currently no experimental technique for measuring α2 in highly-compressed near-roomerature (NRT) superconductors. In this paper, we propose to advance McMillan's approach (1968 Phys Rev 167 331), which utilises the Debye temperature θ (an integrated parameter for the full phonon spectrum), deduced via the fit of experimentally measured temperature-dependent resistance data R(T) to the Bloch-Grüneisen equation for highly-compressed black phosphorous, boron, GeAs, SiH4, HxS, DxS, LaHx, and LaDy. By utilizing the relations between T c, Tθ, and the electron-phonon coupling strength constant λ e-ph (which can be computed from first-principles calculations), it is possible to affirm/disprove the electron-phonon coupling mechanism in given superconductors. We show that computed λ e-ph for highly-compressed black phosphorous, boron, GeAs, SiH4, and for one sample of LaH10 are in a good agreement with λ e-ph values deduced from experimental data. A remarkable constancy of θ= 1531 \pm 70 for H3S at different ageing stages is also found. We also show that if the phonon spectra of two isotopic counterparts share an identical shape (or, in the case of highly-compressed superconductors, the same material at different pressures), then within electron-phonon phenomenology, these materials should obey the relation of Tθ ,1/Tθ,2 = T c,1/T c,2 = ω ln,1/ω ln,2 (where subscripts 1 and 2 designate two isotopic counterparts). We further report that H3S-D3S pair ratios of T c,H3S/T c,D3S = ω ln,H3S/ω ln,D3S = 1.27 are largely different from deduced Tθ,H3S/Tθ,D3S = 1.65. This implies that NRT superconductivity in H3S-D3S systems originates from more than one mechanism, where the electron-phonon coupling lifts T c in H3S vs D3S, but the primary origin for the NRT background of T c ∼ 150 K in both H3S and D3S remains to be discovered. © 2020 IOP Publishing Ltden
dc.format.mimetypeapplication/pdfen
dc.language.isoenen
dc.publisherIOP Publishing Ltden
dc.rightsinfo:eu-repo/semantics/openAccessen
dc.sourceSupercond Sci Technol2
dc.sourceSuperconductor Science and Technologyen
dc.subjectARSENIC COMPOUNDSen
dc.subjectBORONen
dc.subjectCALCULATIONSen
dc.subjectELECTRON CORRELATIONSen
dc.subjectELECTRONSen
dc.subjectGERMANIUM COMPOUNDSen
dc.subjectISOTOPESen
dc.subjectLANTHANUM COMPOUNDSen
dc.subjectPHOSPHORUSen
dc.subjectSILANESen
dc.subjectSILICONen
dc.subjectSUPERCONDUCTING MATERIALSen
dc.subjectSUPERCONDUCTING TRANSITION TEMPERATUREen
dc.subjectDIFFERENT PRESSURESen
dc.subjectELECTRON PHONON COUPLINGSen
dc.subjectELECTRON-PHONON COUPLING STRENGTHSen
dc.subjectEXPERIMENTAL TECHNIQUESen
dc.subjectFIRST-PRINCIPLES CALCULATIONen
dc.subjectINTEGRATED PARAMETERen
dc.subjectITS APPLICATIONSen
dc.subjectMEASURED TEMPERATURESen
dc.subjectELECTRON-PHONON INTERACTIONSen
dc.titleAdvanced McMillan's equation and its application for the analysis of highly-compressed superconductorsen
dc.typeArticleen
dc.typeinfo:eu-repo/semantics/articleen
dc.typeinfo:eu-repo/semantics/publishedVersionen
dc.identifier.doi10.1088/1361-6668/ab953f-
dc.identifier.scopus85091760337-
local.contributor.employeeTalantsev, E.F., M.N. Mikheev 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.issue9-
local.volume33-
dc.identifier.wos000557045200001-
local.contributor.departmentM.N. Mikheev 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.pure13687767-
local.description.order094009-
local.identifier.eid2-s2.0-85091760337-
local.identifier.wosWOS:000557045200001-
Appears in Collections:Научные публикации ученых УрФУ, проиндексированные в SCOPUS и WoS CC

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