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Investigation of the electronic structure and lattice dynamics of the thermoelectric material Na-doped SnSe

机译:热电材料掺Na SnSe的电子结构和晶格动力学研究

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摘要

SnSe has drawn considerable attention on a global scale due to its intrinsic low thermal conductivity and large figure of merit along the b axis. In Na-doped SnSe, further enhancement of the thermoelectric performance has been reported. Using angle-resolved photoemission spectroscopy and inelastic neutron scattering, we have studied how electronic structures and lattice dynamics evolve with temperature in Na-doped SnSe. Our data show that the effective mass of the Se p_z orbital along the Γ-Z direction has a very weak temperature dependence, while the chemical potential shifts significantly along with the increase in the gap size evidenced by infrared absorption measurements. Inelastic neutron scattering reveals one acoustic TA and two low-lying optical (TO1 and TO2) phonon modes. Their temperature-dependent behaviors indicate that the TO1 and TA modes contribute more to the reduction of the lattice thermal conductivity with temperature increases. The estimated value of the lattice thermal conductivity based on the lattice dynamics is significantly larger than that determined by transport measurements, suggesting that extrinsic factors, such as the imperfection of the lattice, could drastically suppress the lattice thermal conductivity. Our data suggest that temperature-dependent properties of both electronic structures and phonon dynamics need to be taken into account for the investigation of the underlying physics of hole-doped SnSe.
机译:SnSe由于其固有的低导热性和沿b轴的优异品质,已在全球范围内引起了相当大的关注。在掺Na的SnSe中,已经报道了热电性能的进一步提高。使用角度分辨光发射光谱和非弹性中子散射,我们研究了掺Na SnSe中电子结构和晶格动力学如何随温度演化。我们的数据表明,沿着Γ-Z方向的Se p_z轨道的有效质量具有非常弱的温度依赖性,而化学势随红外吸收测量结果证明,随着间隙尺寸的增加而发生显着变化。非弹性中子散射揭示了一个声波TA和两个低地光学声波(TO1和TO2)声子模式。它们与温度有关的行为表明,TO1和TA模式随着温度的升高对晶格热导率的降低做出更大的贡献。基于晶格动力学的晶格热导率估计值显着大于通过传输测量确定的值,这表明诸如晶格缺陷的外在因素可以极大地抑制晶格热导率。我们的数据表明,在研究掺杂空穴的SnSe的基本物理特性时,必须考虑电子结构和声子动力学的温度相关特性。

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  • 来源
    《Physical review. B, Condensed Matter And Materals Physics》 |2018年第9期|094305.1-094305.7|共7页
  • 作者单位

    National Synchrotron Radiation Laboratory, University of Science and Technology of China, Hefei, Anhui 230029, People's Republic of China,Institute of Materials Structure Science, KEK, Tokai, Ibaraki 319-1106, Japan;

    National Synchrotron Radiation Laboratory, University of Science and Technology of China, Hefei, Anhui 230029, People's Republic of China;

    Chongqing Institute of Green and Intelligent Technology, Chinese Academy of Sciences, Chongqing 400714, People's Republic of China;

    Institute of Materials Structure Science, KEK, Tokai, Ibaraki 319-1106, Japan;

    Institute of Materials Structure Science, KEK, Tokai, Ibaraki 319-1106, Japan;

    Japan Proton Accelerator Research Complex, Japan Atomic Energy Agency, Tokai, Ibaraki 319-1195, Japan;

    Institute of Materials Structure Science, KEK, Tokai, Ibaraki 319-1106, Japan;

    Institute of Materials Structure Science, KEK, Tsukuba, Ibaraki 305-0801, Japan;

    National Synchrotron Radiation Laboratory, University of Science and Technology of China, Hefei, Anhui 230029, People's Republic of China;

    National Synchrotron Radiation Laboratory, University of Science and Technology of China, Hefei, Anhui 230029, People's Republic of China;

    Japan Proton Accelerator Research Complex, Japan Atomic Energy Agency, Tokai, Ibaraki 319-1195, Japan;

    Chongqing Institute of Green and Intelligent Technology, Chinese Academy of Sciences, Chongqing 400714, People's Republic of China;

    National Synchrotron Radiation Laboratory, University of Science and Technology of China, Hefei, Anhui 230029, People's Republic of China,CAS Key Laboratory of Strongly-coupled Quantum Matter Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China;

    Institute of Materials Structure Science, KEK, Tokai, Ibaraki 319-1106, Japan;

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