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Transparency of graphene and other direct-gap two-dimensional materials

Daniel J. Merthe and Vitaly V. Kresin
Phys. Rev. B 94, 205439 – Published 30 November 2016
Physics logo See Synopsis: Graphene’s Elegant Optics Explained

Abstract

Graphene and other two-dimensional materials display remarkable optical properties, including a simple transparency of T1πα for visible light. Most theoretical rationalizations of this “universal” opacity employ a model coupling light to the electron's crystal momentum and put emphasis on the linear dispersion of the graphene bands. However, such a formulation of interband absorption is not allowable within band structure theory, because it conflates the crystal momentum label with the canonical momentum operator. We show that the physical origin of the optical behavior of graphene can be explained within a straightforward picture with the correct use of canonical momentum coupling. Its essence lies in the two-dimensional character of the density of states rather than in the precise dispersion relation, and therefore the discussion is applicable to other systems such as semiconductor membranes. At higher energies the calculation predicts a peak corresponding to a van Hove singularity as well as a specific asymmetry in the absorption spectrum of graphene, in agreement with previous results.

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  • Received 26 August 2016

DOI:https://doi.org/10.1103/PhysRevB.94.205439

©2016 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Synopsis

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Graphene’s Elegant Optics Explained

Published 30 November 2016

Theoretical calculations anchor graphene’s simple optical absorption in its two-dimensional structure instead of its cone-shaped energy bands.

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Authors & Affiliations

Daniel J. Merthe* and Vitaly V. Kresin

  • Department of Physics and Astronomy, University of Southern California, Los Angeles, California 90089-0484, USA

  • *merthe@usc.edu
  • kresin@usc.edu

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Issue

Vol. 94, Iss. 20 — 15 November 2016

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