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Observation of Dirac state in half-Heusler material YPtBi

The prediction of non-trivial topological electronic states in half-Heusler compounds makes these materials good candidates for discovering new physics and devices as half-Heusler phases harbour a variety of electronic ground states, including superconductivity, antiferromagnetism, and heavy-fermion...

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Detalles Bibliográficos
Autores principales: Hosen, M. Mofazzel, Dhakal, Gyanendra, Dimitri, Klauss, Choi, Hongchul, Kabir, Firoza, Sims, Christopher, Pavlosiuk, Orest, Wiśniewski, Piotr, Durakiewicz, Tomasz, Zhu, Jian-Xin, Kaczorowski, Dariusz, Neupane, Madhab
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group UK 2020
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7378050/
https://www.ncbi.nlm.nih.gov/pubmed/32704042
http://dx.doi.org/10.1038/s41598-020-69284-5
Descripción
Sumario:The prediction of non-trivial topological electronic states in half-Heusler compounds makes these materials good candidates for discovering new physics and devices as half-Heusler phases harbour a variety of electronic ground states, including superconductivity, antiferromagnetism, and heavy-fermion behaviour. Here, we report a systematic studies of electronic properties of a superconducting half-Heusler compound YPtBi, in its normal state, investigated using angle-resolved photoemission spectroscopy. Our data reveal the presence of a Dirac state at the [Formula: see text] point of the Brillouin zone at 500 meV below the Fermi level. We observe the presence of multiple Fermi surface pockets, including two concentric hexagonal and six half-oval shaped pockets at the [Formula: see text] and K points of the Brillouin zone, respectively. Furthermore, our measurements show Rashba-split bands and multiple surface states crossing the Fermi level, this is also supported by the first-principles calculations. Our findings of a Dirac state in YPtBi contribute to the establishing of half-Heusler compounds as a potential platform for novel topological phases.