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
Synchrotrons Utilisation Section, RRCAT Indore 452013 India
Homi Bhabha National Institute Anushakti Nagar Mumbai 400094 India.
RSC Adv. 2020 Dec 9;10(71):43497-43507. doi: 10.1039/d0ra09128f. eCollection 2020 Nov 27.
Crystallographic and electronic structures of phase pure ternary solid solutions of Ni Co O ( = 0 to 1) have been studied using XRD, EXAFS and XAS measurements. The lattice parameter of the cubic rock-salt (RS) Ni Co 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 "", 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 "" is very similar to the variation in the optical gap with "", 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 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.
利用X射线衍射(XRD)、扩展X射线吸收精细结构(EXAFS)和X射线吸收光谱(XAS)测量方法,对NiCoₓO₁₋ₓ(x = 0至1)相纯三元固溶体的晶体结构和电子结构进行了研究。在整个成分范围内,立方岩盐(RS)NiCoₓO₁₋ₓ固溶体的晶格参数随Co含量的增加呈线性增加,并遵循维加德定律。观察到键长(Ni/Co - O、Ni - Ni和Ni - Co)随x呈线性增加,与通过虚拟晶体近似(VCA)确定的键长密切相关,这意味着混合晶体中晶格的局部畸变最小。由漫反射率测量确定的三元固溶体的光学带隙既不随Co成分呈线性变化,也不像许多三元半导体那样出现弯曲。通过在O K边使用XAS探测导带,解释了光学带隙变化的这种趋势。我们观察到,导带边缘起始能量随x的变化与光学带隙随x的变化非常相似,从而清楚地表明导带位置在确定光学带隙中起主导作用。发现在Ni和Co K边测量的XANES光谱中预边峰的强度变化,以及在Ni和Co L边测量的XAS光谱中L峰的强度变化,取决于未占据的O 2p - 金属 - (Ni/Co)3d杂化态和键长。