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Spin fluctuation induced Weyl semimetal state in the paramagnetic phase of EuCd2As2

机译:EuCd2As2顺磁相中自旋涨落诱导的Weyl半金属态

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摘要

Weyl fermions as emergent quasiparticles can arise in Weyl semimetals (WSMs) in which the energy bands are nondegenerate, resulting from inversion or time-reversal symmetry breaking. Nevertheless, experimental evidence for magnetically induced WSMs is scarce. Here, using photoemission spectroscopy, we observe that the degeneracy of Bloch bands is already lifted in the paramagnetic phase of EuCd2As2. We attribute this effect to the itinerant electrons experiencing quasi-static and quasi–long-range ferromagnetic fluctuations. Moreover, the spin-nondegenerate band structure harbors a pair of ideal Weyl nodes near the Fermi level. Hence, we show that long-range magnetic order and the spontaneous breaking of time-reversal symmetry are not essential requirements for WSM states in centrosymmetric systems and that WSM states can emerge in a wider range of condensed matter systems than previously thought.
机译:魏尔费米子作为准准粒子可以出现在魏尔半金属(WSMs)中,其中能带未简并,是由于反演或时间反转对称性破坏造成的。然而,关于磁感应WSM的实验证据很少。在这里,使用光发射光谱法,我们观察到在EuCd2As2的顺磁相中Bloch谱带的简并性已经提高。我们将此影响归因于流动电子经历了准静态和准远距离铁磁波动。此外,自旋简并的能带结构在费米能级附近具有一对理想的Weyl节点。因此,我们表明,远心磁阶和时间反转对称性的自发破坏不是中心对称系统中WSM状态的必要条件,而且WSM状态可以在比以前认为的更广泛的凝聚态系统中出现。

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