Please use this identifier to cite or link to this item: http://localhost:8080/xmlui/handle/123456789/2194
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dc.contributor.authorJoshi, D.C.-
dc.contributor.authorHarish, D.D-
dc.contributor.authorNayak, S.-
dc.contributor.authorRoy, D.-
dc.contributor.authorQureshi, Md-
dc.contributor.authorSaiprasad, R.L.N.-
dc.contributor.authorShiyani, T.-
dc.contributor.authorPamu, D.-
dc.contributor.authorThota, S-
dc.date.accessioned2024-12-30T05:14:13Z-
dc.date.available2024-12-30T05:14:13Z-
dc.date.issued2014-
dc.identifier.citation10.1109/ICEmElec.2014.7151180en_US
dc.identifier.urihttp://localhost:8080/xmlui/handle/123456789/2194-
dc.descriptionNITWen_US
dc.description.abstractTwo-phase nanocomposites comprised of Zn 1-x Ni x O/NiO (0.05 ≤ x ≤ 0.3) were grown by using sol-gel process with hydrated metal acetates as precursors. Thermal decomposition of the co-precipitated oxalate α-ZnNi(C 2 O 4 ) yields wurtzite h.c.p. Zn 1-x Ni x O and f.c.c. NiO together. The X-band electron spin resonance spectra provide the signatures of anisotropic spin interactions with long-range magnetic ordering at 300 K. The temperature variation (120 K ≤ T ≤ 300 K) of the resonance field H R (T) and line-width ΔH PP (T) depicts a clear anomaly across 140 K associated with the blocking/freezing effects and the contribution of additional surface anisotropy (K eff ) present in the system. Both H R (T) and ΔH PP (T) follows the power-law variation δH R = (ΔH PP ) n with n ≃ 2.13, as expected for partially oriented nanocrystallites.en_US
dc.language.isoenen_US
dc.publisher2014 IEEE 2nd International Conference on Emerging Electronics: Materials to Devices, ICEE 2014 - Conference Proceedingsen_US
dc.subjectWide band-gap semiconductor,en_US
dc.subjectElectron-SpinResonanceen_US
dc.titleGrowth mechanism and Electron Spin Resonance Studies of Zn1-xNixO/NiO Two-Phase Nanocompositeen_US
dc.typeOtheren_US
Appears in Collections:Physics



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