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Phonon dispersion relation of single-crystalline β-FeSe

机译:β-FeSe单晶的声子色散关系

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We report on the phonon spectrum probed at the β-FeSe(001) surface by means of high-resolution electron energy-loss spectroscopy (HREELS). Single crystals of β-FeSe are cleaved under ultrahigh-vacuum conditions and are subsequently measured below and above the nematic transition temperature. In total we observe five phonon modes and a phonon cutoff energy of about 40 meV. We identify the origin of each phonon mode based on the selection rules of HREELS and by comparing the experimental results to those of ab initio density functional calculations. The most prominent phonon modes A_(1g), B_(1g), and A_(2u) appear at energies of about 20.5 and 25.6 and 40 meV, respectively. These phonon modes disperse rather weakly while changing the momentum from zero up to the zone boundary, indicating that they are mainly of optical nature. A comparison between our results and the results of ab initio calculations indicates that there must be a mutual interplay between magnetism and lattice dynamics in this compound, similar to the other Fe-based superconductors. Finally, we comment on the role of temperature on the phonon modes probed at the f point. It is observed that both the B_(1g) and A_(2u) phonon modes undergo a downward shift while increasing the temperature from 15 to 300 K. In the case of the A_(2u) mode this shift is about 1.5 meV.
机译:我们通过高分辨率电子能量损失谱(HREELS)报告了在β-FeSe(001)表面探测的声子谱。 β-FeSe的单晶在超高真空条件下裂解,随后在向列转变温度以下和以上进行测量。我们总共观察到五个声子模式和约40 meV的声子截止能量。我们根据HREELS的选择规则并通过将实验结果与从头算密度函数计算的结果进行比较,来确定每种声子模式的起源。最突出的声子模式A_(1g),B_(1g)和A_(2u)分别以大约20.5、25.6和40 meV的能量出现。这些声子模式在将动量从零更改为区域边界时,色散相当弱,表明它们主要具有光学性质。我们的结果与从头算的结果之间的比较表明,该化合物中的磁性和晶格动力学之间必须存在相互作用,这与其他基于Fe的超导体相似。最后,我们评论温度对在f点探测的声子模式的作用。可以看出,B_(1g)和A_(2u)声子模式都发生了向下偏移,同时温度从15 K升高到300K。在A_(2u)模式下,该偏移约为1.5 meV。

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  • 来源
    《Physical review. B, Condensed Matter And Materals Physics》 |2017年第9期|094531.1-094531.6|共6页
  • 作者单位

    Heisenberg Spin-Dynamics Group, Physikalisches Institut, Karlsruhe Institute of Technology, Wolfgang-Gaede-Straße 1, D-76131 Karlsruhe, Germany;

    Heisenberg Spin-Dynamics Group, Physikalisches Institut, Karlsruhe Institute of Technology, Wolfgang-Gaede-Straße 1, D-76131 Karlsruhe, Germany;

    Institut für Festkörperphysik, Karlsruhe Institute of Technology, Hermann-v.-Helmholtz-Platz 1, D-76344 Eggenstein-Leopoldshafen, Germany;

    Institut für Festkörperphysik, Karlsruhe Institute of Technology, Hermann-v.-Helmholtz-Platz 1, D-76344 Eggenstein-Leopoldshafen, Germany;

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