<?xml version="1.0" encoding="UTF-8"?>
<collection>
<dc:dc xmlns:dc="http://purl.org/dc/elements/1.1/" xmlns:invenio="http://invenio-software.org/elements/1.0" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/ http://www.openarchives.org/OAI/2.0/oai_dc.xsd"><dc:identifier>doi:10.1103/PhysRevLett.125.256804</dc:identifier><dc:language>eng</dc:language><dc:creator>Brey, L.</dc:creator><dc:creator>Stauber, T.</dc:creator><dc:creator>Slipchenko, T.</dc:creator><dc:creator>Martín-Moreno, L.</dc:creator><dc:title>Plasmonic Dirac Cone in Twisted Bilayer Graphene</dc:title><dc:identifier>ART-2020-122323</dc:identifier><dc:description>We discuss plasmons of biased twisted bilayer graphene when the Fermi level lies inside the gap. The collective excitations are a network of chiral edge plasmons (CEP) entirely composed of excitations in the topological electronic edge states that appear at the AB-BA interfaces. The CEP form a hexagonal network with a unique energy scale ?p=(e2)/(?0?t0) with t0 the moiré lattice constant and ? the dielectric constant. From the dielectric matrix we obtain the plasmon spectra that has two main characteristics: (i) a diverging density of states at zero energy, and (ii) the presence of a plasmonic Dirac cone at â., ?~?p/2 with sound velocity vD=0.0075c, which is formed by zigzag and armchair current oscillations. A network model reveals that the antisymmetry of the plasmon bands implies that CEP scatter at the hexagon vertices maximally in the deflected chiral outgoing directions, with a current ratio of 4/9 into each of the deflected directions and 1/9 into the forward one. We show that scanning near-field microscopy should be able to observe the predicted plasmonic Dirac cone and its broken symmetry phases.</dc:description><dc:date>2020</dc:date><dc:source>http://zaguan.unizar.es/record/99083</dc:source><dc:doi>10.1103/PhysRevLett.125.256804</dc:doi><dc:identifier>http://zaguan.unizar.es/record/99083</dc:identifier><dc:identifier>oai:zaguan.unizar.es:99083</dc:identifier><dc:relation>info:eu-repo/grantAgreement/ES/DGA/Q-MAD</dc:relation><dc:relation>info:eu-repo/grantAgreement/EC/H2020/785219/EU/Graphene Flagship Core Project 2/GrapheneCore2</dc:relation><dc:relation>This project has received funding from the European Union’s Horizon 2020 research and innovation program under grant agreement No H2020 785219-GrapheneCore2</dc:relation><dc:relation>info:eu-repo/grantAgreement/EC/H2020/881603/EU/Graphene Flagship Core Project 3/GrapheneCore3</dc:relation><dc:relation>This project has received funding from the European Union’s Horizon 2020 research and innovation program under grant agreement No H2020 881603-GrapheneCore3</dc:relation><dc:relation>info:eu-repo/grantAgreement/ES/MINECO/FIS2017-82260-P</dc:relation><dc:relation>info:eu-repo/grantAgreement/ES/MINECO/MAT2017-88358-C3-1-R</dc:relation><dc:relation>info:eu-repo/grantAgreement/ES/MINECO/PGC2018-096955-B-C42</dc:relation><dc:relation>info:eu-repo/grantAgreement/ES/MINECO/PGC2018-097018-B-100</dc:relation><dc:identifier.citation>Physical Review Letters 125, 25 (2020), 256804 [6 pp]</dc:identifier.citation><dc:rights>All rights reserved</dc:rights><dc:rights>http://www.europeana.eu/rights/rr-f/</dc:rights><dc:rights>info:eu-repo/semantics/openAccess</dc:rights></dc:dc>

</collection>