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dc.contributor.authorTalantsev, E. F.en
dc.date.accessioned2024-04-05T16:20:51Z-
dc.date.available2024-04-05T16:20:51Z-
dc.date.issued2023-
dc.identifier.citationTalantsev, EF 2023, 'D-Wave Superconducting Gap Symmetry as a Model for Nb1−xMoxB2 (x = 0.25; 1.0) and WB2 Diborides', Symmetry, Том. 15, № 4, 812. https://doi.org/10.3390/sym15040812harvard_pure
dc.identifier.citationTalantsev, E. F. (2023). D-Wave Superconducting Gap Symmetry as a Model for Nb1−xMoxB2 (x = 0.25; 1.0) and WB2 Diborides. Symmetry, 15(4), [812]. https://doi.org/10.3390/sym15040812apa_pure
dc.identifier.issn2073-8994-
dc.identifier.otherFinal2
dc.identifier.otherAll Open Access, Gold, Green3
dc.identifier.otherhttps://www.scopus.com/inward/record.uri?eid=2-s2.0-85156101919&doi=10.3390%2fsym15040812&partnerID=40&md5=1eff95d9c9831e308b3a21360e01ef5a1
dc.identifier.otherhttps://www.mdpi.com/2073-8994/15/4/812/pdf?version=1679909697pdf
dc.identifier.urihttp://elar.urfu.ru/handle/10995/130444-
dc.description.abstractRecently, Pei et al. (National Science Review 2023, nwad034, 10.1093/nsr/nwad034) reported that ambient pressure (Formula presented.) -MoB2 (space group: (Formula presented.)) exhibits a phase transition to (Formula presented.) -MoB2 (space group: (Formula presented.)) at pressure P~70 GPa, which is a high-temperature superconductor exhibiting (Formula presented.) at P~110 GPa. Although (Formula presented.) -MoB2 has the same crystalline structure as ambient-pressure MgB2 and the superconducting critical temperatures of (Formula presented.) -MoB2 and MgB2 are very close, the first-principles calculations show that in (Formula presented.) -MoB2, the states near the Fermi level, (Formula presented.), are dominated by the d-electrons of Mo atoms, while in MgB2, the p-orbitals of boron atomic sheets dominantly contribute to the states near the (Formula presented.). Recently, Hire et al. (Phys. Rev. B 2022, 106, 174515) reported that the (Formula presented.) -phase can be stabilized at ambient pressure in Nb1−xMoxB2 solid solutions, and that these ternary alloys exhibit (Formula presented.). Additionally, Pei et al. (Sci. China-Phys. Mech. Astron. 2022, 65, 287412) showed that compressed WB2 exhibited (Formula presented.) at P~121 GPa. Here, we aimed to reveal primary differences/similarities in superconducting state in MgB2 and in its recently discovered diboride counterparts, Nb1−xMoxB2 and highly-compressed WB2. By analyzing experimental data reported for P6/mmm-phases of Nb1−xMoxB2 (x = 0.25; 1.0) and highly compressed WB2, we showed that these three phases exhibit d-wave superconductivity. We deduced (Formula presented.) for (Formula presented.) -MoB2, (Formula presented.) for Nb0.75Mo0.25B2, and (Formula presented.) for WB2. We also found that Nb0.75Mo0.25B2 exhibited high strength of nonadiabaticity, which was quantified by the ratio of (Formula presented.), whereas MgB2, α-MoB2, and WB2 exhibited (Formula presented.), which is similar to the (Formula presented.) in pnictides, A15 alloys, Heusler alloys, Laves phase compounds, cuprates, and highly compressed hydrides. © 2023 by the author.en
dc.format.mimetypeapplication/pdfen
dc.language.isoenen
dc.publisherMDPIen
dc.rightsinfo:eu-repo/semantics/openAccessen
dc.rightscc-byother
dc.rights.urihttps://creativecommons.org/licenses/by/4.0/unpaywall
dc.sourceSymmetry2
dc.sourceSymmetryen
dc.subjectHIGH-PRESSURE SUPERCONDUCTIVITYen
dc.subjectNONADIABATIC SUPERCONDUCTORSen
dc.subjectSUPERCONDUCTING DIBORIDESen
dc.subjectSUPERCONDUCTING GAP SYMMETRYen
dc.titleD-Wave Superconducting Gap Symmetry as a Model for Nb1−xMoxB2 (x = 0.25; 1.0) and WB2 Diboridesen
dc.typeArticleen
dc.typeinfo:eu-repo/semantics/articleen
dc.type|info:eu-repo/semantics/publishedVersionen
dc.identifier.doi10.3390/sym15040812-
dc.identifier.scopus85156101919-
local.contributor.employeeTalantsev, E.F., Institute of Metal Physics, Ural Branch, Russian Academy of Sciences, 18, S. Kovalevskoy St, Ekaterinburg, 620108, Russian Federation, NANOTECH Centre, Ural Federal University, 19 Mira St, Ekaterinburg, 620002, Russian Federationen
local.issue4-
local.volume15-
dc.identifier.wos000988888600001-
local.contributor.departmentInstitute of Metal Physics, Ural Branch, Russian Academy of Sciences, 18, S. Kovalevskoy St, Ekaterinburg, 620108, Russian Federationen
local.contributor.departmentNANOTECH Centre, Ural Federal University, 19 Mira St, Ekaterinburg, 620002, Russian Federationen
local.identifier.pure38493510-
local.description.order812-
local.identifier.eid2-s2.0-85156101919-
local.identifier.wosWOS:000988888600001-
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