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X-ray absorption and optical spectroscopy studies of (Mg1-xAlx)B-2

dc.citation.epage0en_US
dc.citation.issue9en_US
dc.citation.spage0en_US
dc.citation.volume68en_US
dc.citation.woscount10en_US
dc.contributor.authorYang, HDen_US
dc.contributor.authorLiu, HLen_US
dc.contributor.authorLin, JYen_US
dc.contributor.authorKuo, MXen_US
dc.contributor.authorHo, PLen_US
dc.contributor.authorChen, JMen_US
dc.contributor.authorJung, CUen_US
dc.contributor.authorPark, MSen_US
dc.contributor.authorLee, SIen_US
dc.contributor.department物理研究所zh_TW
dc.contributor.departmentInstitute of Physicsen_US
dc.date.accessioned2019-04-03T06:38:20Z
dc.date.available2019-04-03T06:38:20Z
dc.date.issued2003-09-01en_US
dc.description.abstractX-ray absorption spectroscopy and optical reflectance measurements have been carried out to elucidate the evolution of the electronic structure in (Mg1-xAlx) B-2 for x=0.0, 0.1, 0.2, 0.3, and 0.4. The important role of B 2psigma hole states to superconductivity has been identified, and the decrease in the hole carrier number is quantitatively determined. The rate of the decrease in the hole concentration agrees well with the theoretical calculations. On the other hand, while the evolution of the electronic structure is gradual through the doping range, T-c suppression is most significant at x=0.4. These results suggest that the superstructure in (Mg1-xAlx)B-2, in addition to the sigma holes, can affect the lattice dynamics and contributes to the T-c suppression effect. Other possible explanations like the topological change of the sigma band Fermi surface are also discussed.en_US
dc.identifier.doi10.1103/PhysRevB.68.092505en_US
dc.identifier.issn2469-9950en_US
dc.identifier.journalPHYSICAL REVIEW Ben_US
dc.identifier.urihttp://dx.doi.org/10.1103/PhysRevB.68.092505en_US
dc.identifier.urihttps://ir.lib.nycu.edu.tw/handle/11536/27540
dc.identifier.wosnumberWOS:000185717600023en_US
dc.language.isoen_USen_US
dc.titleX-ray absorption and optical spectroscopy studies of (Mg1-xAlx)B-2en_US
dc.typeArticleen_US

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