Please use this identifier to cite or link to this item: https://dspace.iiti.ac.in/handle/123456789/8119
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dc.contributor.authorWarshi, M. Kamalen_US
dc.date.accessioned2022-03-17T01:00:00Z-
dc.date.accessioned2022-03-21T11:15:10Z-
dc.date.available2022-03-17T01:00:00Z-
dc.date.available2022-03-21T11:15:10Z-
dc.date.issued2019-
dc.identifier.citationJoshi, D. C., Pramanik, P., Warshi, M. K., Ghosh, S., Meher, A., Dasari, K., & Thota, S. (2019). Role of phase transition in the dielectric and magnetic properties of na containing NiO. Journal of Physics and Chemistry of Solids, 130, 154-164. doi:10.1016/j.jpcs.2019.02.012en_US
dc.identifier.issn0022-3697-
dc.identifier.otherEID(2-s2.0-85062348434)-
dc.identifier.urihttps://doi.org/10.1016/j.jpcs.2019.02.012-
dc.identifier.urihttps://dspace.iiti.ac.in/handle/123456789/8119-
dc.description.abstractIn this study, we systematically investigated the phase transition (cubic (90°) → rhombohedral (60.01°)) and its role in the electronic structure, dielectric, and magnetic behavior of Ni 1−x Na x O (0.02≤x≤ 0.2). X-ray photoelectron spectroscopy indicated non-local screening of the divalent Ni by oxygen and monovalent sodium ions together with giant multiplet splitting. At 310 K, the longitudinal optical phonon mode (500 cm −1 ) dominated over all the vibrational excitations, but for the dilute dispersion of Na, the transverse optical phonon mode (455 cm −1 ) exhibited the highest intensity among all the modes. Even at a very low level (x∼ 0.02) of Na substitution, the intensity of the 2-magnon mode (1530 cm −1 ) was significantly suppressed. The onset of the structural transition and antiferromagnetic Néel temperature (T N ) shifted to a high temperature region with moderate Na substitution, which has significant implications for the dependence of the relative dielectric permittivity (ε R (T)) and magnetic susceptibility (χ mag (T)) on the temperature. The dependence of the ac-resistivity ρ ac (T, f) on the temperature and frequency followed Mott's variable range-hopping mechanism for charge carriers between the localized states, where the activation energies were highly dependent on the spin (S = 1/2) of the type-II antiferromagnetic system. The magnetization isotherms (M–H) were analyzed using a modified Langevin function M=M o L([Formula presented])+χ a H and we extracted T N for the Ni 1−x Na x O system. © 2019 Elsevier Ltden_US
dc.language.isoenen_US
dc.publisherElsevier Ltden_US
dc.sourceJournal of Physics and Chemistry of Solidsen_US
dc.subjectAntiferromagnetismen_US
dc.subjectElectronic structureen_US
dc.subjectMagnetic susceptibilityen_US
dc.subjectMetal ionsen_US
dc.subjectNickel oxideen_US
dc.subjectPermittivityen_US
dc.subjectPhononsen_US
dc.subjectX ray photoelectron spectroscopyen_US
dc.subjectAntiferromagnetic systemsen_US
dc.subjectDielectric and magnetic propertiesen_US
dc.subjectLongitudinal optical phononsen_US
dc.subjectMagnetization isothermsen_US
dc.subjectRelative dielectric permittivityen_US
dc.subjectStructural transitionsen_US
dc.subjectTransverse optical phononsen_US
dc.subjectVibrational excitationen_US
dc.subjectActivation energyen_US
dc.titleRole of phase transition in the dielectric and magnetic properties of Na containing NiOen_US
dc.typeJournal Articleen_US
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