词条 | Dirac cone |
释义 |
As an object with three dimensions, Dirac cones are a feature of two-dimensional materials or surface states, based on a linear dispersion relation between energy and the two components of the crystal momentum kx and ky. However, this concept can be extended to three dimensions, where Dirac semimetals are defined by a linear dispersion relation between energy and kx, ky, and kz. In k-space, this shows up as a hypercone, which have doubly degenerate bands which also meet at Dirac points. Dirac semimetals contain both time reversal and spacial inversion symmetry; when one of these is broken, the Dirac points are split into two constituent Weyl points, and the material becomes a Weyl semimetal.[6][7] In 2014, direct observation of the Dirac semimetal band structure using ARPES was conducted on the Dirac semimetal cadmium arsenide.[8] References1. ^{{cite web |url=http://www.wpi-aimr.tohoku.ac.jp/en/aimresearch/highlight/2011/20110829_000812.html |title=Superconductors: Dirac cones come in pairs |newspaper=Tohoku University Advanced Institute for Materials Research - Research Highlights|date=29 Aug 2011 |author= |accessdate=2 Mar 2018}} {{quantum-stub}}2. ^{{cite journal|url=https://www.equipes.lps.u-psud.fr/Montambaux/reprints/178-interband-tunneling.pdf|title=Interband tunneling near the merging transition of Dirac cones|publisher=Physical Review A|author1=Jean-Noël Fuchs|author2=Lih-King Lim|author3=Gilles Montambaux|year=2012|volume=86|page=063613|doi=10.1103/PhysRevA.86.063613|arxiv=1210.3703|bibcode=2012PhRvA..86f3613F}} 3. ^{{cite web|url=https://www.nature.com/articles/nature04233|title=Two-dimensional gas of massless Dirac fermions in graphene|publisher=Nature|author=K. S. Novoselov, A. K. Geim, S. V. Morozov, D. Jiang, M. I. Katsnelson, I. V. Grigorieva, S. V. Dubonos & A. A. Firsov|date=10 Nov 2005|accessdate=2 Mar 2018}} 4. ^{{cite web |url=http://phys.org/news/2015-04-two-dimensional-dirac-materials-properties-rarity.html |title=Two-dimensional Dirac materials: Structure, properties, and rarity |newspaper=Phys.org |date= |author= |accessdate= May 25, 2016}} 5. ^{{cite journal|url=https://journals.aps.org/prb/abstract/10.1103/PhysRevB.80.075431|title=Angle-resolved photoemission study of the graphite intercalation compound KC8: A key to graphene|authors=A. Grüneis, C. Attaccalite, A. Rubio, D. V. Vyalikh, S. L. Molodtsov, J. Fink, R. Follath, W. Eberhardt, B. Büchner, and T. Pichler|year=2009|journal=Physical Review B|volume=80|issue=7|page=075431|doi=10.1103/PhysRevB.80.075431|bibcode=2009PhRvB..80g5431G}} 6. ^{{cite journal|last1=Schoop|first1=Leslie M.|last2=Ali|first2=Mazhar N.| last3=Straßer|first3=Carola|last4=Topp|first4=Andreas|last5=Varykhalov|first5=Andrei|last6=Marchenko|first6=Dmitry|last7=Duppel|first7=Viola|last8=Parkin|first8=Stuart S. P.|last9=Lotsch|first9=Bettina V.|last10=Ast|first10=Christian R.|title=Dirac cone protected by non-symmorphic symmetry and three-dimensional Dirac line node in ZrSiS|journal=Nature Communications|volume=7|issue=1|year=2016|issn=2041-1723|doi=10.1038/ncomms11696}} 7. ^{{cite web|url=http://www.mit.edu/~soljacic/Weyl_nat-phot.pdf|title=Weyl points and line nodes in gyroid photonic crystals|publisher=Nature Photonics|author=Ling Lu, Liang Fu, John D. Joannopoulos and Marin Soljacˇic|date=17 Mar 2013|accessdate=2 Mar 2018}} 8. ^{{cite journal|last1=Borisenko|first1=Sergey|last2=Gibson|first2=Quinn|last3=Evtushinsky|first3=Danil|last4=Zabolotnyy|first4=Volodymyr|last5=Büchner|first5=Bernd|last6=Cava|first6=Robert J.|title=Experimental Realization of a Three-Dimensional Dirac Semimetal|journal=Physical Review Letters|volume=113|issue=2|year=2014|issn=0031-9007|doi=10.1103/PhysRevLett.113.027603}} 1 : Electronic band structures |
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