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Structural, optical and electronic properties of Ni(1−x)Co(x)O in the complete composition range

Crystallographic and electronic structures of phase pure ternary solid solutions of Ni(1−x)Co(x)O (x = 0 to 1) have been studied using XRD, EXAFS and XAS measurements. The lattice parameter of the cubic rock-salt (RS) Ni(1−x)Co(x)O solid solutions increases linearly with increasing Co content and fo...

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Autores principales: Baraik, Kiran, Bhakar, Ashok, Srihari, V., Bhaumik, Indranil, Mukherjee, C., Gupta, Mukul, Yadav, A. K., Tiwari, Pragya, Phase, D. M., Jha, S. N., Singh, S. D., Ganguli, Tapas
Formato: Online Artículo Texto
Lenguaje:English
Publicado: The Royal Society of Chemistry 2020
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9058517/
https://www.ncbi.nlm.nih.gov/pubmed/35519712
http://dx.doi.org/10.1039/d0ra09128f
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author Baraik, Kiran
Bhakar, Ashok
Srihari, V.
Bhaumik, Indranil
Mukherjee, C.
Gupta, Mukul
Yadav, A. K.
Tiwari, Pragya
Phase, D. M.
Jha, S. N.
Singh, S. D.
Ganguli, Tapas
author_facet Baraik, Kiran
Bhakar, Ashok
Srihari, V.
Bhaumik, Indranil
Mukherjee, C.
Gupta, Mukul
Yadav, A. K.
Tiwari, Pragya
Phase, D. M.
Jha, S. N.
Singh, S. D.
Ganguli, Tapas
author_sort Baraik, Kiran
collection PubMed
description Crystallographic and electronic structures of phase pure ternary solid solutions of Ni(1−x)Co(x)O (x = 0 to 1) have been studied using XRD, EXAFS and XAS measurements. The lattice parameter of the cubic rock-salt (RS) Ni(1−x)Co(x)O solid solutions increases linearly with increasing Co content and follows Vegard's law, in the complete composition range. A linear increase in the bond lengths (Ni/Co–O, Ni–Ni and Ni–Co) with “x”, closely following the bond lengths determined from virtual crystal approximation (VCA), is observed, which implies that there is only a minimal local distortion of the lattice in the mixed crystal. The optical gap of the ternary solid solution determined from diffuse reflectivity measurements shows neither a linear variation with Co composition nor bowing, as observed in many ternary semiconductors. This trend in the variation of optical gaps is explained by probing the conduction band using XAS at the O K-edge. We have observed that the variation in the onset energy of the conduction band edge with “x” is very similar to the variation in the optical gap with “x”, thus clearly indicating the dominant role played by the conduction band position in determining the optical gap. The variation in the intensities of the pre-edge peak in the XANES spectra measured at Ni and Co K-edges, and the L(1/2) peak in XAS spectra measured at Ni and Co L-edges, is found to depend on the unoccupied O 2p-metal-(Ni/Co) 3d hybridized states and the bond lengths.
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spelling pubmed-90585172022-05-04 Structural, optical and electronic properties of Ni(1−x)Co(x)O in the complete composition range Baraik, Kiran Bhakar, Ashok Srihari, V. Bhaumik, Indranil Mukherjee, C. Gupta, Mukul Yadav, A. K. Tiwari, Pragya Phase, D. M. Jha, S. N. Singh, S. D. Ganguli, Tapas RSC Adv Chemistry Crystallographic and electronic structures of phase pure ternary solid solutions of Ni(1−x)Co(x)O (x = 0 to 1) have been studied using XRD, EXAFS and XAS measurements. The lattice parameter of the cubic rock-salt (RS) Ni(1−x)Co(x)O solid solutions increases linearly with increasing Co content and follows Vegard's law, in the complete composition range. A linear increase in the bond lengths (Ni/Co–O, Ni–Ni and Ni–Co) with “x”, closely following the bond lengths determined from virtual crystal approximation (VCA), is observed, which implies that there is only a minimal local distortion of the lattice in the mixed crystal. The optical gap of the ternary solid solution determined from diffuse reflectivity measurements shows neither a linear variation with Co composition nor bowing, as observed in many ternary semiconductors. This trend in the variation of optical gaps is explained by probing the conduction band using XAS at the O K-edge. We have observed that the variation in the onset energy of the conduction band edge with “x” is very similar to the variation in the optical gap with “x”, thus clearly indicating the dominant role played by the conduction band position in determining the optical gap. The variation in the intensities of the pre-edge peak in the XANES spectra measured at Ni and Co K-edges, and the L(1/2) peak in XAS spectra measured at Ni and Co L-edges, is found to depend on the unoccupied O 2p-metal-(Ni/Co) 3d hybridized states and the bond lengths. The Royal Society of Chemistry 2020-12-09 /pmc/articles/PMC9058517/ /pubmed/35519712 http://dx.doi.org/10.1039/d0ra09128f Text en This journal is © The Royal Society of Chemistry https://creativecommons.org/licenses/by/3.0/
spellingShingle Chemistry
Baraik, Kiran
Bhakar, Ashok
Srihari, V.
Bhaumik, Indranil
Mukherjee, C.
Gupta, Mukul
Yadav, A. K.
Tiwari, Pragya
Phase, D. M.
Jha, S. N.
Singh, S. D.
Ganguli, Tapas
Structural, optical and electronic properties of Ni(1−x)Co(x)O in the complete composition range
title Structural, optical and electronic properties of Ni(1−x)Co(x)O in the complete composition range
title_full Structural, optical and electronic properties of Ni(1−x)Co(x)O in the complete composition range
title_fullStr Structural, optical and electronic properties of Ni(1−x)Co(x)O in the complete composition range
title_full_unstemmed Structural, optical and electronic properties of Ni(1−x)Co(x)O in the complete composition range
title_short Structural, optical and electronic properties of Ni(1−x)Co(x)O in the complete composition range
title_sort structural, optical and electronic properties of ni(1−x)co(x)o in the complete composition range
topic Chemistry
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9058517/
https://www.ncbi.nlm.nih.gov/pubmed/35519712
http://dx.doi.org/10.1039/d0ra09128f
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