Please use this identifier to cite or link to this item: http://hdl.handle.net/123456789/2735
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dc.contributor.authorBalodhi, A.-
dc.contributor.authorSingh, Yogesh-
dc.date.accessioned2020-12-07T07:12:28Z-
dc.date.available2020-12-07T07:12:28Z-
dc.date.issued2015-
dc.identifier.citationJournal of Physics Condensed Matter, 27 (48)en_US
dc.identifier.other10.1088/0953-8984/27/48/485603-
dc.identifier.urihttps://iopscience.iop.org/article/10.1088/0953-8984/27/48/485603/meta-
dc.identifier.urihttp://hdl.handle.net/123456789/2735-
dc.descriptionOnly IISERM authors are available in the record.-
dc.description.abstractWe report 23Na nuclear magnetic resonance (NMR) and zero-field (ZF) and longitudinal-field (LF) muon spin relaxation (μSR) measurements of the depleted hyperkagome compounds Na4−xIr3O8 (x  =  0.3 and 0.7), which undergo an insulator-semimetal transition as a function of x. The 23Na spin-lattice relaxation rates, $T_{1}^{-1}$ , follow a T2.5 power law behavior at accessible temperatures of T  =  120–350 K. A substantial temperature dependence of $T_{1}^{-1}$ indicates the presence of gapped excitations at elevated temperatures through the transition to a semimetallic phase. ZF-μSR results reveal that hole-doping leads to a melting of quasi-static order to a dynamically fluctuating state. The very slow muon depolarization rate which varies hardly with temperature indicates that spins are close to an itinerant limit in the largest doping x  =  0.7. The dynamic relaxation rates extracted from the LF-μSR spectra show a three-dimensional diffusive transport. Our combined NMR and μSR results suggest the occurrence of intriguing spin and charge excitations across the insulator-semimetal transition.en_US
dc.language.isoen_USen_US
dc.publisherInstitute of Physics Publishingen_US
dc.subjectSpin dynamicsen_US
dc.subjectNa4−xIr3O8en_US
dc.subjectx  =  0.3 and 0.7en_US
dc.subject23Na NMR and μSRen_US
dc.titleSpin dynamics in Na4-xIr3O8 (x = 0.3 and 0.7) investigated by 23Na NMR and μsRen_US
dc.typeArticleen_US
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