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首页> 外文期刊>Physical review, B >Interplay between bandwidth-controlled and filling-controlled pressure-induced Mott insulator to metal transition in the molecular compound [Au(Et-thiazdt)(2)]
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Interplay between bandwidth-controlled and filling-controlled pressure-induced Mott insulator to metal transition in the molecular compound [Au(Et-thiazdt)(2)]

机译:带宽控制和填充控制的压力诱导的MOTT绝缘体与分子化合物中金属转变之间的相互作用[Au(et-thiazdt)(2)]

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摘要

Optical properties of the quasi-two-dimensional single-component molecular Mott insulator [Au(Et-thiazdt)2] (Et-thiazdt = N-ethyl-1,3-thiazoline-2-thione-4,5-dithiolate) have been investigated under pressure at room temperature. At 1.5 GPa, [Au(Et-thiazdt)2] undergoes an insulator to metal transition (IMT). Optical conductivity spectra exhibit a clear Drude peak at high pressure. In addition, we observed a clear anisotropy of pressure-induced modifications of the electronic structure. With increasing pressure, along the molecule stacks, a strong increase of the spectral weight below 1 eV is observed, while in the transverse direction, it remains barely constant with a redistribution from midinfrared to low energy. Besides the increase of the singly occupied molecular orbital (SOMO) bandwidth, calculations show that the SOMO-1 bands cross the Fermi level at the transition. Moreover, we have calculated the optical conductivity as a function of pressure to provide a picture of the compound physics under 1 eV. Our results indicate that the pressure-induced IMT is simultaneously due to a bandwidth and a band-filling phenomenon that imply both Mott physics and uncorrelated charge carriers.
机译:准二维单组分分子Mott绝缘体的光学性质[Au(et-thiazdt)2](Et-thiazdt = N-乙基-1,3-噻唑啉-2-倍硫醚)具有在室温下在压力下进行了研究。在1.5GPa,[Au(et-thiazdt)2]经过金属转换(IMT)的绝缘体。光电导率光谱在高压下表现出清晰的磨牙峰。此外,我们观察到了一种清晰的电子结构修改的各向异性。随着压力的增加,沿着分子堆叠,观察到低于1eV的光谱重量的强大增加,而在横向方向上,它仍然几乎不恒定,从中小三射到低能量。除了单独占用的分子轨道(SOMO)带宽的增加外,计算表明,SOMO-1带在过渡时穿过费米水平。此外,我们已经计算了作为压力的函数的光导率,以提供1eV下的复合物理学的图像。我们的结果表明,压力引起的IMT由于带宽和填充现象而暗示Mott物理和不相关的电荷载体的带宽现象。

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  • 来源
    《Physical review, B》 |2018年第3期|共7页
  • 作者单位

    Univ Tours UFR Sci GREMAN CNRS UMR CEA 7347 Parc Grandmont F-37200 Tours France;

    Univ Tours UFR Sci GREMAN CNRS UMR CEA 7347 Parc Grandmont F-37200 Tours France;

    Univ Tours UFR Sci GREMAN CNRS UMR CEA 7347 Parc Grandmont F-37200 Tours France;

    Univ Rennes CNRS ISCR UMR 6226 F-35000 Rennes France;

    Univ Roma Sapienza CNR IOM Ple Aldo Moro 2 I-00185 Rome Italy;

    Elettra Sincrotrone Trieste SCpA AREA Sci Pk I-34149 Trieste Italy;

    Univ Tours UFR Sci GREMAN CNRS UMR CEA 7347 Parc Grandmont F-37200 Tours France;

    Univ Tours UFR Sci GREMAN CNRS UMR CEA 7347 Parc Grandmont F-37200 Tours France;

    Univ Tours UFR Sci GREMAN CNRS UMR CEA 7347 Parc Grandmont F-37200 Tours France;

    Univ Tours UFR Sci GREMAN CNRS UMR CEA 7347 Parc Grandmont F-37200 Tours France;

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  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 固体物理学;
  • 关键词

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