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首页> 外文期刊>International Journal of Quantum Chemistry >Coupled In/Te and Ni/vacancy ordering and the modulated crystal structure of a B8 type, Ni3 +/- xIn1-yTe2+y solid solution phase
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Coupled In/Te and Ni/vacancy ordering and the modulated crystal structure of a B8 type, Ni3 +/- xIn1-yTe2+y solid solution phase

机译:In / Te和Ni /空位耦合以及B8型Ni3 +/- xIn1-yTe2 + y固溶体相的调制晶体结构

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The commensurate superstructures of a NiAs/Ni2In type parent structure, Ni3.32InTe2 and Ni3.12In0.86Te2.14 (q = gamma[0 0 1]*, gamma = 2/3) as well as one dimensionally incommensurate structure of Ni31nTe2 (gamma = 0.71) were refined from neutron powder diffraction data (R-wp = 4.77%, 4.53% and 4.91 % for the three structures, respectively, at 298 K). The commensurate structures were refined in the P6(3)/mmc space group (c = 3c(NiAs)). The stacking sequence at the hcp array is -In/Te/Te/- and the trigonal bipyrainidal site within the In layer, Ni(2), is partially occupied while it is empty in the Te layers. The octahedral position in between the In and Te layers, Ni(1a), is fully occupied while the octahedral position in between two adjacent Te layers, Ni(1b), is partially occupied. With decreasing In and Ni content, the modulation wave vector,, was found to increase continuously until gamma = 1. From this, crenel functions to describe the whole homogeneity range of the solid solution were constructed with the length of the atomic domains Delta(Te) = gamma (and hence Delta(In) = Delta(Ni) = 1-gamma) and Delta(Ni(1b)) = gamma/2 (and hence Delta(Ni(1a)) = 1-gamma/2) which were then used for the refinement of the incommensurate structure of Ni3InTe2. The corresponding effect in real space is that the single In layers separating double layers of Te, occur less frequent when y in increasing until at gamma = 1 the CdI2 type structure of Ni1+xTe2 is reached. (C) 2007 Elsevier Inc. All rights reserved.
机译:NiAs / Ni2In型母体结构Ni3.32InTe2和Ni3.12In0.86Te2.14(q = gamma [0 0 1] *,gamma = 2/3)的同等上层结构以及Ni31nTe2( γ= 0.71)是根据中子粉末衍射数据(在298 K下三个结构的R-wp = 4.77%,4.53%和4.91%)精制而成的。在P6(3)/ mmc空间组(c = 3c(NiAs))中完善了相应的结构。在hcp数组处的堆叠顺序为-In / Te / Te /-,并且In层中的三角形双锥体部分Ni(2)被部分占据,而Te层中为空。 In和Te层之间的八面体位置Ni(1a)被完全占据,而两个相邻Te层之间的八面体位置Ni(1b)被部分占据。随着In和Ni含量的降低,调制波矢量不断增加,直到γ=1。由此,构造了描述原子固溶体整个均质范围的克里尔函数,其原子域为Delta(Te )=伽玛(因此Delta(In)= Delta(Ni)= 1-gamma)和Delta(Ni(1b))=伽玛/ 2(因此Delta(Ni(1a))= 1-gamma / 2)其中然后将其用于细化Ni3InTe2的不相称结构。实际空间中的相应效果是,当y增大时,分隔Te的双层的单In层出现的频率降低,直到在γ= 1时达到Ni1 + xTe2的CdI2型结构为止。 (C)2007 Elsevier Inc.保留所有权利。

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