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首页> 外文期刊>Journal of the Physical Society of Japan >Holes in the valence band of superconducting boron-doped diamond film studied by soft X-ray absorption and emission spectroscopy
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Holes in the valence band of superconducting boron-doped diamond film studied by soft X-ray absorption and emission spectroscopy

机译:用软X射线吸收和发射光谱研究超导掺硼金刚石薄膜价带中的孔

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摘要

Carbon- and boron-2p states of superconducting and non-superconducting boron-doped diamond (BDD) samples are measured using soft X-ray emission and absorption spectroscopy (XES and XAS) near C- and B-K edges. The electronic structure of B 2p does not show a marked boron-doping dependence, except that a. considerable amount of in-gap state in empty states is observed. In C-K XAS spectra, two peaks H and I are observed around the Fermi level. The H peak is attributed to 2p state of carbon first-nearest neighboring to the dopant boron atoms (INN-C), and the I peak to 2p state of carbon further than INN-C from an impurity boron. Incoherent (normal-excitation) XES spectra do not show a large chemical shift by B-doping, but its intensity just below the valence band maximum (VBM) decreases with B-doping. It cannot be interpreted within a simple rigid band model. An elastic peak of I-excited C-K XES spectrum and the width of I-peak of C-K XAS spectrum suggest that impurity state is localized in non-superconducting BDD but is not in superconducting BDD. Namely impurity state of superconducting BDD is merged with the valence band, and holes in the merged state play an important role in the occurrence of superconductivity of BDD.
机译:使用C和B-K边缘附近的软X射线发射和吸收光谱法(XES和XAS)测量了超导和非超导掺硼金刚石(BDD)样品的碳和硼2p态。 B 2p的电子结构没有显示出明显的硼掺杂依赖性,除了a。在空状态下观察到相当大的间隙状态。在C-K XAS光谱中,在费米能级附近观察到两个峰H和I。 H峰归因于与掺杂剂硼原子(INN-C)相邻的碳最接近的2p态,而I峰归因于来自杂质硼的比INN-C更远的碳的2p态。非相干(正态激发)XES光谱未显示出通过B掺杂产生的大化学位移,但其强度恰好在价带最大值(VBM)以下,随B掺杂而降低。无法在简单的刚性带模型中解释它。 I激发的C-K XES谱的弹性峰和C-K XAS谱的I峰的宽度表明,杂质态位于非超导BDD中,而不在超导BDD中。即,超导BDD的杂质状态与价带合并,并且处于合并状态的空穴在BDD的超导电性的发生中起重要作用。

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