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DC Field | Value | Language |
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dc.contributor.author | Warshi, M. Kamal | en_US |
dc.date.accessioned | 2022-03-17T01:00:00Z | - |
dc.date.accessioned | 2022-03-21T11:15:10Z | - |
dc.date.available | 2022-03-17T01:00:00Z | - |
dc.date.available | 2022-03-21T11:15:10Z | - |
dc.date.issued | 2019 | - |
dc.identifier.citation | Joshi, 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.2019.02.012 | en_US |
dc.identifier.issn | 0022-3697 | - |
dc.identifier.other | EID(2-s2.0-85062348434) | - |
dc.identifier.uri | https://doi.org/10.1016/j.jpcs.2019.02.012 | - |
dc.identifier.uri | https://dspace.iiti.ac.in/handle/123456789/8119 | - |
dc.description.abstract | In 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 Ltd | en_US |
dc.language.iso | en | en_US |
dc.publisher | Elsevier Ltd | en_US |
dc.source | Journal of Physics and Chemistry of Solids | en_US |
dc.subject | Antiferromagnetism | en_US |
dc.subject | Electronic structure | en_US |
dc.subject | Magnetic susceptibility | en_US |
dc.subject | Metal ions | en_US |
dc.subject | Nickel oxide | en_US |
dc.subject | Permittivity | en_US |
dc.subject | Phonons | en_US |
dc.subject | X ray photoelectron spectroscopy | en_US |
dc.subject | Antiferromagnetic systems | en_US |
dc.subject | Dielectric and magnetic properties | en_US |
dc.subject | Longitudinal optical phonons | en_US |
dc.subject | Magnetization isotherms | en_US |
dc.subject | Relative dielectric permittivity | en_US |
dc.subject | Structural transitions | en_US |
dc.subject | Transverse optical phonons | en_US |
dc.subject | Vibrational excitation | en_US |
dc.subject | Activation energy | en_US |
dc.title | Role of phase transition in the dielectric and magnetic properties of Na containing NiO | en_US |
dc.type | Journal Article | en_US |
Appears in Collections: | Department of Physics |
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