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首页> 外文期刊>Physical review. B, Condensed Matter And Materals Physics >Hard x-ray photoemission study of the temperature-induced valence transition system EuNi_2(Si_(1-x)Ge_x)_2
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Hard x-ray photoemission study of the temperature-induced valence transition system EuNi_2(Si_(1-x)Ge_x)_2

机译:温度诱导的价态跃迁体系EuNi_2(Si_(1-x)Ge_x)_2的硬X射线光发射研究

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摘要

We investigated the bulk-derived electronic structure of the temperature-induced valence transition system EuNi_2(Si_(1-x)Ge_x)_2 (x = 0.70, 0.79, and 0.82) by means of hard x-ray photoemission spectroscopy (HAXPES). The HAXPES spectra clearly show distinct temperature dependencies in the spectral intensities of the Eu~(2+) and Eu~(3+) 3d components. For x = 0.70, the changes in the Eu~(2+) and Eu~(3+) 3d spectral components with temperature reflect a continuous valence transition, whereas the sudden changes for x = 0.79 and 0.82 reflect first-order valence transitions. The Eu 3d spectral shapes for all x and particularly the drastic changes in the Eu~(3+) 3d feature with temperature are validated by a theoretical calculation based on the single-impurity Anderson model (SIAM). SIAM analysis reveals that the valence transition for each x is controlled by the c-f hybridization strength and the charge-transfer energy. Furthermore, the c-f hybridization strength governs the valence transition of this system, which is either first order or continuous, consistent with Kondo volume collapse.
机译:我们通过硬X射线光电子能谱(HAXPES)研究了温度诱导的价态跃迁体系EuNi_2(Si_(1-x)Ge_x)_2(x = 0.70、0.79和0.82)的本体衍生电子结构。 HAXPES光谱清楚地显示Eu〜(2+)和Eu〜(3+)3d组分的光谱强度具有明显的温度依赖性。对于x = 0.70,Eu〜(2+)和Eu〜(3+)3d光谱分量随温度的变化反映了连续的价态跃迁,而x = 0.79和0.82的突然变化反映了一阶价态跃迁。通过基于单杂质安德森模型(SIAM)的理论计算,验证了所有x的Eu 3d光谱形状,尤其是Eu〜(3+)3d特征随温度的急剧变化。 SIAM分析表明,每个x的价态跃迁均受c-f杂交强度和电荷转移能的控制。此外,c-f杂交强度决定了该系统的价态跃迁,该价态跃迁是一阶的或连续的,与近藤的体积崩溃一致。

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  • 来源
    《Physical review. B, Condensed Matter And Materals Physics》 |2017年第4期|045106.1-045106.7|共7页
  • 作者单位

    Graduate School of Engineering, Osaka Prefecture University, Sakai 599-8531, Japan;

    Graduate School of Engineering, Osaka Prefecture University, Sakai 599-8531, Japan,Hiroshima Synchrotron Radiation Center, Hiroshima University, Higashi-Hiroshima 739-0046, Japan;

    Graduate School of Engineering, Osaka Prefecture University, Sakai 599-8531, Japan;

    Graduate School of Engineering, Osaka Prefecture University, Sakai 599-8531, Japan;

    Hiroshima Synchrotron Radiation Center, Hiroshima University, Higashi-Hiroshima 739-0046, Japan;

    Graduate School of Science, Hiroshima University, Higashi-Hiroshima 739-8526, Japan Synchrotron SOLEIL, L'Orme des Merisiers,BP48 Saint-Aubin, 91192 Gif-sur-Yvette, France;

    Synchrotron X-ray Station at SPring-8, National Institute for Materials Science (NIMS), Hyogo 679-5148, Japan,Quantum Beam Unit, National Institute for Materials Science (NIMS), Tsukuba 305-0047, Japan;

    Graduate School of Science, Kyushu University, Fukuoka 819-0395, Japan;

    Graduate School of Science, Kyushu University, Fukuoka 819-0395, Japan;

    Graduate School of Engineering, Osaka Prefecture University, Sakai 599-8531, Japan;

    Hiroshima Synchrotron Radiation Center, Hiroshima University, Higashi-Hiroshima 739-0046, Japan;

    Hiroshima Synchrotron Radiation Center, Hiroshima University, Higashi-Hiroshima 739-0046, Japan;

    Hiroshima Synchrotron Radiation Center, Hiroshima University, Higashi-Hiroshima 739-0046, Japan;

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