Please use this identifier to cite or link to this item: http://hdl.handle.net/123456789/3492
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dc.contributor.authorSingh, Yogesh-
dc.date.accessioned2021-01-04T04:26:31Z-
dc.date.available2021-01-04T04:26:31Z-
dc.date.issued2012-
dc.identifier.citationPhysical Review B - Condensed Matter and Materials Physics, 85(17)en_US
dc.identifier.otherhttps://doi.org/10.1103/PhysRevB.85.174509-
dc.identifier.urihttps://journals.aps.org/prb/abstract/10.1103/PhysRevB.85.174509-
dc.identifier.urihttp://hdl.handle.net/123456789/3492-
dc.descriptionOnly IISERM authors are available in the record.-
dc.description.abstractThe Fermi surfaces (FS's) and band dispersions of EuRh 2As 2 have been investigated using angle-resolved photoemission spectroscopy. The results in the high-temperature paramagnetic state are in good agreement with the full-potential linearized augmented-plane-wave calculations, especially in the context of the shape of the two-dimensional FS's and band dispersion around the Γ (0,0) and X (π,π) points. Interesting changes in band folding are predicted by the theoretical calculations below the magnetic transition temperature T N≈47 K. However, by comparing the FS's measured at 60 and 40 K, we did not observe any signature of this transition at the Fermi energy, indicating a very weak coupling of the electrons to the ordered magnetic moments or strong fluctuations. Furthermore, the FS does not change across the temperature (≈25 K) where changes are observed in the Hall coefficient. Notably, the Fermi surface deviates drastically from the usual FS of the superconducting iron-based AFe 2As 2 parent compounds, including the absence of nesting between the Γ and X FS pockets.en_US
dc.language.isoenen_US
dc.publisherAmerican Physical Societyen_US
dc.subjectSpectroscopyen_US
dc.subjectFermi surfacesen_US
dc.subjectTemperatureen_US
dc.titleExperimental and theoretical electronic structure of EuRh 2 As 2en_US
dc.typeArticleen_US
Appears in Collections:Research Articles

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