<HashMap><database>biostudies-literature</database><scores/><additional><submitter>Le C</submitter><funding>European Research Council</funding><pagination>8311-8315</pagination><full_dataset_link>https://www.ebi.ac.uk/biostudies/studies/S-EPMC6099897</full_dataset_link><repository>biostudies-literature</repository><omics_type>Unknown</omics_type><volume>115(33)</volume><pubmed_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.</pubmed_abstract><journal>Proceedings of the National Academy of Sciences of the United States of America</journal><pubmed_title>Dirac semimetal in &lt;i>β&lt;/i>-CuI without surface Fermi arcs.</pubmed_title><pmcid>PMC6099897</pmcid><funding_grant_id>336012</funding_grant_id><pubmed_authors>Li Y</pubmed_authors><pubmed_authors>Zhang FC</pubmed_authors><pubmed_authors>Hu J</pubmed_authors><pubmed_authors>Thomale R</pubmed_authors><pubmed_authors>Le C</pubmed_authors><pubmed_authors>Wu X</pubmed_authors><pubmed_authors>Qin S</pubmed_authors></additional><is_claimable>false</is_claimable><name>Dirac semimetal in &lt;i>β&lt;/i>-CuI without surface Fermi arcs.</name><description>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.</description><dates><release>2018-01-01T00:00:00Z</release><publication>2018 Aug</publication><modification>2026-05-06T06:44:57.517Z</modification><creation>2025-05-18T12:16:53.354Z</creation></dates><accession>S-EPMC6099897</accession><cross_references><pubmed>30061416</pubmed><doi>10.1073/pnas.1803599115</doi></cross_references></HashMap>