用硼替代硅对α-Nb5Si3 的影响:通过理论和实验方法了解 Nb5Si2B 的构成特性

Michał Falkowski, Jakub Kaczkowski, Grażyna Chełkowska, Andrzej Kowalczyk
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摘要

我们结合密度泛函理论(DFT)计算和实验方法,研究了 Nb5Si2B 化合物的结构、弹性、振动和电子特性。我们将研究结果与具有两个非等效 Si 位点(即 Si(4a)和 Si(8h))的母体化合物 Nb5Si3 进行了比较。弹性常数和声子频谱分析表明,Nb5Si2B 分别具有机械稳定性和动力学稳定性。在声子计算的基础上,我们评估了不同位点占有率下的理论恒定体积晶格比热(CV),并将其与实验比热(Cp)测量值进行了比较。我们发现,对于 B 位于 Si(8h)位的 Nb5Si2B,理论和实验结果非常一致,这与计算得出的形成能相吻合。此外,我们还进行了 DFT 计算,旨在显示和比较 Nb5Si3 和 Nb5Si2B 费米水平 (EF) 附近的总 DOS。Nb5Si2B 的 XPS 价带 (VB) 主要由分别位于 - 8.7 和 - 1.7 eV 的两个特征峰所主导。根据 DFT 计算,- 1.7 eV 处的尖锐主峰来自 Nb 4d 态,而位于 - 8.7 eV 处的较小较宽的主峰主要来自与 Nb 4d 态弱杂化的 Si 3s 态。因此,在- 12 eV到EF的结合能范围内,大部分贡献来自铌4d态,而来自硅和B原子的贡献在这一区域非常小。利用 XPS 技术还确定了 Nb 3d、Si 2s、2p 和 B 1s 的核心水平。
本文章由计算机程序翻译,如有差异,请以英文原文为准。

The Effect of Silicon Substitution by Boron for the α-Nb5Si3: INSIGHTS into the Constitutive Properties of Nb5Si2B Through Theory and Experimental Approach

The Effect of Silicon Substitution by Boron for the α-Nb5Si3: INSIGHTS into the Constitutive Properties of Nb5Si2B Through Theory and Experimental Approach

We investigated the structural, elastic, vibrational, and electronic properties of the Nb5Si2B compound combining density functional theory (DFT) calculations and experimental methods. We compared our results with the parent compound Nb5Si3 with two non-equivalent Si sites namely Si(4a) and Si(8h). The analysis of elastic constants and phonon spectra indicate that Nb5Si2B is respectively mechanically and dynamically stable. Based on the phonon calculation we evaluate the theoretical constant volume lattice specific heat (CV) for different site occupancies and compare it with experimental specific heat (Cp) measurements. We found an excellent agreement between theoretical and experimental results for Nb5Si2B with the B at the Si(8h) site, which agrees with the calculated formation energy. In addition, we also performed DFT calculations aimed at showing and comparing the total DOS near the Fermi level (EF) for Nb5Si3 and Nb5Si2B. The XPS valence band (VB) of the Nb5Si2B is largely dominated by two characteristic peaks at − 8.7 and − 1.7 eV, respectively. Based on DFT calculations, it follows that the main sharp peak at − 1.7 eV comes as a contribution from Nb 4d states, while the smaller and broader one located at − 8.7 eV results mainly from Si 3s states weakly hybridized with Nb 4d states. In this connection, the majority contribution in the binding energy range from − 12 eV to the EF comes from Nb 4d states, while the contribution from Si and B atoms is very small in this region. The core levels of Nb 3d, Si 2s, 2p, and B 1s were also identified using the XPS technique.

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