Please use this identifier to cite or link to this item: http://hdl.handle.net/123456789/2431
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dc.contributor.authorBalodhi, A.-
dc.contributor.authorSingh, Yogesh-
dc.date.accessioned2020-12-01T08:36:45Z-
dc.date.available2020-12-01T08:36:45Z-
dc.date.issued2016-
dc.identifier.citationPhysical Review B, 94(15).en_US
dc.identifier.otherhttps://doi.org/10.1103/PhysRevB.94.155153-
dc.identifier.urihttps://journals.aps.org/prb/abstract/10.1103/PhysRevB.94.155153-
dc.identifier.urihttp://hdl.handle.net/123456789/2431-
dc.descriptionOnly IISERM authors are available in the record.-
dc.description.abstractCombining Raman scattering measurements with mean-field calculations of the Raman response, we show that Kitaev-like magnetic exchange is dominant in the hyperkagome iridate Na 4 Ir 3 O 8 . In the measurements we observe a broad Raman band at ∼ 3500 cm − 1 with a bandwidth ∼ 1700 cm − 1 . Calculations of the Raman response of the Kitaev-Heisenberg model on the hyperkagome lattice shows that the experimental observations are consistent with the calculated Raman response where the Kitaev exchange interaction ( J K ) is much larger than the Heisenberg term J 1 ( J 1 / J K ∼ 0.1 ). A comparison with the theoretical model gives an estimate of the Kitaev exchange interaction parameter.en_US
dc.language.isoenen_US
dc.publisherAmerican Physical Societyen_US
dc.subjectRaman responseen_US
dc.subjectCalculationsen_US
dc.subjectMeasurementsen_US
dc.titleSpin liquid like Raman signatures in the hyperkagome iridate Na 4 Ir 3 O 8en_US
dc.typeArticleen_US
Appears in Collections:Research Articles

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