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      Possible permanent Dirac- to Weyl-semimetal phase transition by ion implantation

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          Abstract

          Three-dimensional (3D) topological semimetals (TSMs) are a new class of Dirac materials that can be viewed as 3D graphene and are referred to as Dirac semimetals (DSMs) or Weyl semimetals (WSMs) depending on whether time reversal symmetry and/or inversion symmetry are protected, respectively. Despite some interesting results on Dirac- to Weyl-semimetal phase transitions under conditions of low temperature or strong magnetic field (B), all of them are reversible phenomena. Here, we report for the first time a possible permanent transition in a single TSM by ion implantation. A Dirac- to Weyl-semimetal phase transition in a Bi 0.96Sb 0.04 DSM results from inversion-symmetry breaking induced by implantation with nonmagnetic Au ions for implant fluences ( ϕ G) ≥ 3.2 × 10 16 Au cm −2. This phenomenon is evidenced by the ϕ G-dependent behavior of the Raman spectra and quantum-oscillation parameters extracted from magnetoresistance (MR) measurements, which show abrupt changes at ϕ G ≥ 3.2 × 10 16 Au cm −2. The verification of the transition is further supported by observations of negative MR in the longitudinal B // electric field orientation, indicating the existence of a chiral anomaly in Weyl fermions induced by implantation with nonmagnetic Au ions. In contrast, implantation with magnetic Mn ions exhibits no such particular behavior. Our findings demonstrate the first realization of a possible permanent DSM-to-WSM phase transition in a single material by the simple approach of implantation using nonmagnetic elements.

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          Quantum Spin Hall Effect in Graphene

          We study the effects of spin orbit interactions on the low energy electronic structure of a single plane of graphene. We find that in an experimentally accessible low temperature regime the symmetry allowed spin orbit potential converts graphene from an ideal two-dimensional semimetallic state to a quantum spin Hall insulator. This novel electronic state of matter is gapped in the bulk and supports the transport of spin and charge in gapless edge states that propagate at the sample boundaries. The edge states are nonchiral, but they are insensitive to disorder because their directionality is correlated with spin. The spin and charge conductances in these edge states are calculated and the effects of temperature, chemical potential, Rashba coupling, disorder, and symmetry breaking fields are discussed.
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            Spin-Orbit Interaction and Magnetoresistance in the Two Dimensional Random System

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              Weyl and Dirac semimetals in three-dimensional solids

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                Author and article information

                Contributors
                Journal
                NPG Asia Materials
                NPG Asia Mater
                Springer Science and Business Media LLC
                1884-4049
                1884-4057
                December 2022
                April 08 2022
                December 2022
                : 14
                : 1
                Article
                10.1038/s41427-022-00380-w
                7d8f0052-bb1f-457f-9b71-8b50a31523f6
                © 2022

                https://creativecommons.org/licenses/by/4.0

                https://creativecommons.org/licenses/by/4.0

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