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Dirac semimetal in β-CuI without surface Fermi arcs.


ABSTRACT: Anomalous surface states with Fermi arcs are commonly considered to be a fingerprint of Dirac semimetals (DSMs). In contrast to Weyl semimetals, however, Fermi arcs of DSMs are not topologically protected. Using first-principles calculations, we predict that β-cuprous iodide (β-CuI) is a peculiar DSM whose surface states form closed Fermi pockets instead of Fermi arcs. In such a fermiological Dirac semimetal, the deformation mechanism from Fermi arcs to Fermi pockets stems from a large cubic term preserving all crystal symmetries and from the small energy difference between the surface and bulk Dirac points. The cubic term in β-CuI, usually negligible in prototypical DSMs, becomes relevant because of the particular crystal structure. As such, we establish a concrete material example manifesting the lack of topological protection for surface Fermi arcs in DSMs.

SUBMITTER: Le C 

PROVIDER: S-EPMC6099897 | biostudies-literature | 2018 Aug

REPOSITORIES: biostudies-literature

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Dirac semimetal in <i>β</i>-CuI without surface Fermi arcs.

Le Congcong C   Wu Xianxin X   Qin Shengshan S   Li Yinxiang Y   Thomale Ronny R   Zhang Fu-Chun FC   Hu Jiangping J  

Proceedings of the National Academy of Sciences of the United States of America 20180730 33


Anomalous surface states with Fermi arcs are commonly considered to be a fingerprint of Dirac semimetals (DSMs). In contrast to Weyl semimetals, however, Fermi arcs of DSMs are not topologically protected. Using first-principles calculations, we predict that β-cuprous iodide (β-CuI) is a peculiar DSM whose surface states form closed Fermi pockets instead of Fermi arcs. In such a fermiological Dirac semimetal, the deformation mechanism from Fermi arcs to Fermi pockets stems from a large cubic ter  ...[more]

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