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AO(A = Mn)、AO(A = Sc、Cr和Mn)以及AO(A = Ti和V)的K边X射线吸收近边结构(XANES)光谱中,金红石型和锐钛矿型与温度相关的预边峰强度。

Rutile- and anatase-type temperature-dependent pre-edge peak intensities in K-edge XANES spectra for AO (A = Mn), AO (A = Sc, Cr and Mn) and AO (A = Ti and V).

作者信息

Tobase Tsubasa, Yoshiasa Akira, Hiratoko Tatsuya, Nakatsuka Akihiko

机构信息

Graduate School of Sciences and Technology, Kumamoto University, Chuoku Kurokami 2-39-1, Kumamoto 860-8555, Japan.

Advanced Materials Science and Engineering, Yamaguchi University, Ube, Yamaguchi 755-8611, Japan.

出版信息

J Synchrotron Radiat. 2018 Jul 1;25(Pt 4):1129-1134. doi: 10.1107/S1600577518006902. Epub 2018 Jun 14.

Abstract

Pre-edge peaks in 3d transition-metal element (Sc, Ti, V, Cr and Mn) K-edge XANES (X-ray absorption near-edge structure) spectra in AO (A = Ti and V), AO (A = Sc, Cr and Mn) and AO (A = Mn) are measured at various temperatures. Quantitative comparisons for the XANES spectra were investigated by using absorption intensity invariant point normalization. The energy position of the difference peak (D peak) is obtained from the difference between the low- and high-temperature XANES spectra. There are two kinds of temperature dependence for pre-edge peak intensity: rutile- and anatase-type. The true temperature dependence of a transition to each orbital is obtained from the difference spectrum. In both anatase and rutile, the pre-edge peak positions of A2 and A3 are clearly different from the D1- and D2-peak positions. The A1 peak-top energies in both phases of VO differ from the D1 peak-top energies. The D-peak energy position determined by the difference spectrum should represent one of the true energies for the transition to an independent orbital. The peak-top positions for pre-edge peaks in XANES do not always represent the true energy for independent transitions to orbitals because several orbital transitions overlap with similar energies. This work suggests that deformation vibration (bending mode) is effective in determining the temperature dependence for the D-peak intensity.

摘要

在不同温度下测量了AO(A = Ti和V)、AO(A = Sc、Cr和Mn)以及AO(A = Mn)中3d过渡金属元素(Sc、Ti、V、Cr和Mn)K边X射线吸收近边结构(XANES)光谱中的预边峰。通过使用吸收强度不变点归一化对XANES光谱进行了定量比较。差谱峰(D峰)的能量位置由低温和高温XANES光谱之间的差值获得。预边峰强度存在两种温度依赖性:金红石型和锐钛矿型。从差谱中获得了向每个轨道跃迁的真实温度依赖性。在锐钛矿和金红石中,A2和A3的预边峰位置与D1和D2峰位置明显不同。VO两个相中的A1峰顶能量与D1峰顶能量不同。由差谱确定的D峰能量位置应代表跃迁到独立轨道的真实能量之一。XANES中预边峰的峰顶位置并不总是代表跃迁到轨道的真实能量,因为几个轨道跃迁的能量相似,相互重叠。这项工作表明,变形振动(弯曲模式)对于确定D峰强度的温度依赖性是有效的。

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