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Universal scattering response across the type-II Weyl semimetal phase diagram

机译:II型Weyl半金属相图的通用散射响应

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摘要

The discovery of Weyl semimetals represents a significant advance in topological band theory. They paradigmatically enlarged the classification of topological materials to gapless systems while simultaneously providing experimental evidence for the long-sought Weyl fermions. Beyond fundamental relevance, their high mobility, strong magnetoresistance, and the possible existence of even more exotic effects, such as the chiral anomaly, make Weyl semimetals a promising platform to develop radically new technology. Fully exploiting their potential requires going beyond the mere identification of materials and calls for a detailed characterization of their functional response, which is severely complicated by the coexistence of surface- and bulk-derived topologically protected quasiparticles, i.e., Fermi arcs and Weyl points, respectively. Here, we focus on the type-II Weyl semimetal class in which we find a stoichiometry-dependent phase transition from a trivial to a nontrivial regime. By exploring the two extreme cases of the phase diagram, we demonstrate the existence of a universal response of both surface and bulk states to perturbations. We show that quasiparticle interference patterns originate from scattering events among surface arcs. Analysis reveals that topologically nontrivial contributions are strongly suppressed by spin texture. We also show that scattering at localized impurities can generate defect-induced quasiparticles sitting close to the Weyl point energy. These give rise to strong peaks in the local density of states, which lift the Weyl node, significantly altering the pristine low-energy spectrum. Remarkably, by comparing the WTe_2 and the MoTe_2 cases we found that scattering response and topological transition are not directly linked. Visualizing the existence of a universal microscopic response to scattering has important consequences for understanding the unusual transport properties of this class of materials. Overall, our observations provide a unifying picture of the type-II Weyl phase diagram.
机译:Weyl半金属的发现代表了拓扑带理论的重大进步。他们在范式上将拓扑材料的分类扩大到了无间隙系统,同时为长期寻求的Weyl费米子提供了实验证据。除了基本意义外,它们的高迁移率,强大的磁阻以及可能存在的更奇特的效应(例如手性异常)使Weyl半金属成为开发全新技术的有前途的平台。充分利用它们的潜力不仅需要对材料进行识别,还需要对其功能响应进行详细的表征,而表面和本体衍生的拓扑受保护的准粒子(即分别为费米弧和魏尔点)的共存会严重地使其复杂化。 。在这里,我们集中于II型Weyl半金属类,在该类中,我们发现了化学计量相关的从平凡态到非平凡态的相变。通过探索相图的两种极端情况,我们证明了表面状态和整体状态对微扰的普遍响应的存在。我们表明,准粒子干涉图案源自表面弧之间的散射事件。分析显示,自旋纹理强烈抑制了拓扑上的重要贡献。我们还表明,在局部杂质处的散射会产生缺陷诱导的准粒子,这些粒子位于接近Weyl点能量的位置。这些会在状态的局部密度中产生强烈的峰值,从而使Weyl节点升高,从而极大地改变了原始的低能谱。值得注意的是,通过比较WTe_2和MoTe_2的情况,我们发现散射响应和拓扑转换没有直接联系。可视化普遍存在的对散射的微观响应,对于理解此类材料的异常传输特性具有重要意义。总体而言,我们的观察提供了II型Weyl相图的统一图片。

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  • 来源
    《Physical review. B, Condensed Matter And Materals Physics》 |2018年第7期|075106.1-075106.9|共9页
  • 作者单位

    Peter Gruenberg Institut and Institute for Advanced Simulation, Forschungszentrum Juelich and JARA, 52425 Juelich, Germany;

    Institute of Physics, Ecole Polytechnique Federate de Lausanne, 1015 Lausanne, Switzerland,Swiss Light Source, Paul Scherrer Institute, 5232 Villigen-PSI, Switzerland;

    Physikalisches Institut, Experimentelle Physik II, Universitaet Wuerzburg, Am Hubland, D-97074 Wuerzburg, Germany;

    Institute of Physics, Ecole Polytechnique Federate de Lausanne, 1015 Lausanne, Switzerland,Swiss Light Source, Paul Scherrer Institute, 5232 Villigen-PSI, Switzerland;

    Institute of Physics, Ecole Polytechnique Federate de Lausanne, 1015 Lausanne, Switzerland,Swiss Light Source, Paul Scherrer Institute, 5232 Villigen-PSI, Switzerland;

    Institute of Physics, Ecole Polytechnique Federate de Lausanne, 1015 Lausanne, Switzerland,Swiss Light Source, Paul Scherrer Institute, 5232 Villigen-PSI, Switzerland;

    Institute of Physics, Ecole Polytechnique Federate de Lausanne, 1015 Lausanne, Switzerland;

    Institute of Physics, Ecole Polytechnique Federate de Lausanne, 1015 Lausanne, Switzerland;

    Institute of Physics, Ecole Polytechnique Federate de Lausanne, 1015 Lausanne, Switzerland;

    Physikalisches Institut, Experimentelle Physik II, Universitaet Wuerzburg, Am Hubland, D-97074 Wuerzburg, Germany;

    Institute of Physics, Ecole Polytechnique Federate de Lausanne, 1015 Lausanne, Switzerland,Swiss Light Source, Paul Scherrer Institute, 5232 Villigen-PSI, Switzerland;

    Peter Gruenberg Institut and Institute for Advanced Simulation, Forschungszentrum Juelich and JARA, 52425 Juelich, Germany;

    Peter Gruenberg Institut and Institute for Advanced Simulation, Forschungszentrum Juelich and JARA, 52425 Juelich, Germany;

    Physikalisches Institut, Experimentelle Physik II, Universitaet Wuerzburg, Am Hubland, D-97074 Wuerzburg, Germany;

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