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首页> 外文期刊>Physical review. B, Condensed Matter And Materals Physics >Spectroscopic evidence of topological phase transition in the three-dimensional Dirac semimetal Cd_3(As_(1-x)P_x)_2
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Spectroscopic evidence of topological phase transition in the three-dimensional Dirac semimetal Cd_3(As_(1-x)P_x)_2

机译:三维Dirac半金属Cd_3(As_(1-x)P_x)_2的拓扑相变的光谱学证据

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摘要

We study the low-energy electronic structure of three-dimensional Dirac semimetal, Cd_3(As_(1-x)P_x)_2 [x = O and 0.34(3)], by employing angle-resolved photoemission spectroscopy (ARPES). We observe that the bulk Dirac states in Cd_3(As_(0.66)P_(0.34))_2 are gapped out with an energy of 0.23 eV, contrary to the parent Cd_3As_2 in which the gapless Dirac states have been observed. Thus, our results confirm the earlier predicted topological phase transition in Cd_3As_2 with perturbation. We further notice that the critical P substitution concentration, at which the two Dirac points that are spread along the c-axis in Cd_3As_2 form a single Dirac point at Γ, is much lower [x_c(P) < 0.34(3)] than the predicted value of x_c(P) = 0.9. Therefore, our results suggest that the nontrivial band topology of Cd_3As_2 is remarkably sensitive to the P substitution and can only survive over a narrow substitution range, i.e., 0 ≤ x(P) < 0.34(3).
机译:我们通过采用角分辨光发射光谱法(ARPES)研究了三维Dirac半金属Cd_3(As_(1-x)P_x)_2 [x = O and 0.34(3)]的低能电子结构。我们观察到Cd_3(As_(0.66)P_(0.34))_ 2中的体Dirac态的能量为0.23 eV,这与观察到无间隙Dirac态的母体Cd_3As_2相反。因此,我们的结果证实了Cd_3As_2具有扰动的早期预测拓扑相变。我们进一步注意到,临界P替代浓度比在Cd_3As_2中沿c轴分布的两个Dirac点在Γ处形成单个Dirac点的浓度低得多[x_c(P)<0.34(3)]。 x_c(P)的预测值= 0.9。因此,我们的结果表明,Cd_3As_2的非平凡的拓扑结构对P替换非常敏感,并且只能在一个狭窄的替换范围内生存,即0≤x(P)<0.34(3)。

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  • 来源
    《Physical review. B, Condensed Matter And Materals Physics》 |2018年第8期|085145.1-085145.5|共5页
  • 作者单位

    Leibniz Institute for Solid State Research, IFW Dresden, D-01171 Dresden, Germany,Solid State and Structural Chemistry Unit, Indian Institute of Science, Bangalore, Karnataka-560012, India,S. N. Bose National Center for Basic Sciences, Block-JD, Salt lake, Kolkata-700098, India;

    Leibniz Institute for Solid State Research, IFW Dresden, D-01171 Dresden, Germany,Lebedev Physical Institute, Russian Academy of Sciences, 119991 Moscow, Russia;

    Leibniz Institute for Solid State Research, IFW Dresden, D-01171 Dresden, Germany;

    Leibniz Institute for Solid State Research, IFW Dresden, D-01171 Dresden, Germany;

    Leibniz Institute for Solid State Research, IFW Dresden, D-01171 Dresden, Germany;

    Diamond Light Source, Harwell Campus, Didcot OX11 0DE, United Kingdom;

    Leibniz Institute for Solid State Research, IFW Dresden, D-01171 Dresden, Germany,Lomonosov Moscow State University, 119991 Moscow, Russia;

    Lomonosov Moscow State University, 119991 Moscow, Russia;

    Leibniz Institute for Solid State Research, IFW Dresden, D-01171 Dresden, Germany,A. E. Arbuzov Institute of Organic and Physical Chemistry, federal Research Center, Kazan Scientific Center of the Russian Academy of Sciences, Kazan, Russia;

    Leibniz Institute for Solid State Research, IFW Dresden, D-01171 Dresden, Germany;

    Leibniz Institute for Solid State Research, IFW Dresden, D-01171 Dresden, Germany;

    Leibniz Institute for Solid State Research, IFW Dresden, D-01171 Dresden, Germany;

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