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dc.contributor.authorZimmer, D.
dc.contributor.authorRuiz Fuertes, Javier 
dc.contributor.authorMorgenroth, W
dc.contributor.authorFriedrich, A.
dc.contributor.authorBayarjargal, L.
dc.contributor.authorHaussühl, Eiken
dc.contributor.authorSantamaría Pérez, David
dc.contributor.authorFrischkorn, S.
dc.contributor.authorMilman, V.
dc.contributor.authorWinkler, B.
dc.contributor.otherUniversidad de Cantabriaes_ES
dc.date.accessioned2024-06-04T18:39:43Z
dc.date.available2024-06-04T18:39:43Z
dc.date.issued2018-04-13
dc.identifier.issn1098-0121
dc.identifier.issn1550-235X
dc.identifier.issn2469-9950
dc.identifier.issn2469-9969
dc.identifier.otherMAT2016-75586-C4-1/3-Pes_ES
dc.identifier.otherMAT2015-71070-REDCes_ES
dc.identifier.urihttps://hdl.handle.net/10902/32988
dc.description.abstractThe high-pressure behavior of monoclinic (P21/c) α-chalcocite, Cu2S, was investigated at ambient temperature by single-crystal x-ray diffraction, electrical resistance measurements, and optical absorption spectroscopy up to 16 GPa. The experiments were complemented by density-functional-theory-based calculations. Single-crystal x-ray diffraction data show that monoclinic α-chalcocite undergoes two pressure-induced first-order phase transitions at ∼3.1 and ∼7.1 GPa. The crystal structure of the first high-pressure polymorph, HP1, was solved and refined in space group P21/c with a = 10.312(4) A˚, b = 6.737(3) A˚, c = 7.305(1) A˚ and β = 100.17(2)◦ at 6.2(3) GPa. The crystal structure of the second high-pressure polymorph, HP2, was solved and refined in space group P21/c with a = 6.731(4) A˚, b = 6.689(2) A˚, c = 6.967(8) A˚, and β = 93.18(3)◦ at 7.9(4) GPa. Electrical resistance measurements upon compression and optical absorption experiments upon decompression show that the structural changes in α-chalcocite are accompanied by changes of the electrical and optical properties. Upon pressure release, the band gap Eg of α-chalcocite (1.24 eV at ambient conditions) widens across the first structural phase transition, going from 1.24 eV at 2.2 GPa (α-chalcocite) to 1.35 eV at 2.6 GPa (HP1), and closes significantly across the second phase transition, going from 1.32 eV at 4.4 GPa (HP1) to 0.87 eV at 4.9 GPa (HP2). The electrical resistance shows similar behavior: its highest value is for the first high-pressure polymorph (HP1), and its lowest value is for the second high-pressure polymorph (HP2) of α-chalcocite. These results are interpreted on the basis of calculated electronic band structures.es_ES
dc.description.sponsorshipFinancial support from the Goethe-University Frankfurt am Main, the DFG (Wi 1232), and the BMBF (05K16RFA, 05K16RFB) is gratefully acknowledged. J.R.-F. and D.S.-P. acknowledge the Spanish Ministry of Economy and Competitiveness (MINECO) for the Juan de la Cierva (IJCI-2014- 20513) and Ramón y Cajal (RYC-2014-15643) programs, respectively. MINECO is also acknowledged for financial support from Projects No.MAT2016-75586-C4-1/3-P and No. MAT2015-71070-REDC (MALTA Consolider).es_ES
dc.format.extent9 p.es_ES
dc.language.isoenges_ES
dc.publisherAmerican Physical Societyes_ES
dc.rights© American Physical Societyes_ES
dc.sourcePhysical Review B, 2018, 97(13), 134111es_ES
dc.titlePressure-induced changes of the structure and properties of monoclinic α-chalcocite Cu₂Ses_ES
dc.typeinfo:eu-repo/semantics/articlees_ES
dc.relation.publisherVersionhttps://doi.org/10.1103/PhysRevB.97.134111es_ES
dc.rights.accessRightsopenAccesses_ES
dc.identifier.DOI10.1103/PhysRevB.97.134111
dc.type.versionpublishedVersiones_ES


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