Berry phase and pseudospin winding number in bilayer graphene

Ever since the novel quantum Hall effect in bilayer graphene was discovered, and explained by a Berry phase of 2π [ K. S. Novoselov et al. Nat. Phys. 2 177 (2006)], it has been widely accepted that the low-energy electronic wave function in this system is described by a nontrivial Berry phase of 2π,...

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Main Authors: Marzari, Nicola, Park, Cheol Hwan
Other Authors: Massachusetts Institute of Technology. Department of Materials Science and Engineering
Format: Article
Language:en_US
Published: American Physical Society (APS) 2012
Online Access:http://hdl.handle.net/1721.1/69581
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author Marzari, Nicola
Park, Cheol Hwan
author2 Massachusetts Institute of Technology. Department of Materials Science and Engineering
author_facet Massachusetts Institute of Technology. Department of Materials Science and Engineering
Marzari, Nicola
Park, Cheol Hwan
author_sort Marzari, Nicola
collection MIT
description Ever since the novel quantum Hall effect in bilayer graphene was discovered, and explained by a Berry phase of 2π [ K. S. Novoselov et al. Nat. Phys. 2 177 (2006)], it has been widely accepted that the low-energy electronic wave function in this system is described by a nontrivial Berry phase of 2π, different from the zero phase of a conventional two-dimensional electron gas. Here, we show that (i) the relevant Berry phase for bilayer graphene is not different from that for a conventional two-dimensional electron gas (as expected, given that Berry phase is only meaningful modulo 2π), and (ii) what is actually observed in the quantum Hall measurements is not the absolute value of the Berry phase but the pseudospin winding number.
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spelling mit-1721.1/695812022-09-30T14:16:53Z Berry phase and pseudospin winding number in bilayer graphene Marzari, Nicola Park, Cheol Hwan Massachusetts Institute of Technology. Department of Materials Science and Engineering Marzari, Nicola Park, Cheol Hwan Ever since the novel quantum Hall effect in bilayer graphene was discovered, and explained by a Berry phase of 2π [ K. S. Novoselov et al. Nat. Phys. 2 177 (2006)], it has been widely accepted that the low-energy electronic wave function in this system is described by a nontrivial Berry phase of 2π, different from the zero phase of a conventional two-dimensional electron gas. Here, we show that (i) the relevant Berry phase for bilayer graphene is not different from that for a conventional two-dimensional electron gas (as expected, given that Berry phase is only meaningful modulo 2π), and (ii) what is actually observed in the quantum Hall measurements is not the absolute value of the Berry phase but the pseudospin winding number. Intel Corporation 2012-03-02T19:50:22Z 2012-03-02T19:50:22Z 2011-11 2011-10 Article http://purl.org/eprint/type/JournalArticle 1098-0121 1550-235X http://hdl.handle.net/1721.1/69581 Park, Cheol-Hwan, and Nicola Marzari. “Berry Phase and Pseudospin Winding Number in Bilayer Graphene.” Physical Review B 84.20 (2011): n. pag. Web. 2 Mar. 2012. © 2011 American Physical Society en_US http://dx.doi.org/10.1103/PhysRevB.84.205440 Physical Review B Article is made available in accordance with the publisher's policy and may be subject to US copyright law. Please refer to the publisher's site for terms of use. application/pdf American Physical Society (APS) APS
spellingShingle Marzari, Nicola
Park, Cheol Hwan
Berry phase and pseudospin winding number in bilayer graphene
title Berry phase and pseudospin winding number in bilayer graphene
title_full Berry phase and pseudospin winding number in bilayer graphene
title_fullStr Berry phase and pseudospin winding number in bilayer graphene
title_full_unstemmed Berry phase and pseudospin winding number in bilayer graphene
title_short Berry phase and pseudospin winding number in bilayer graphene
title_sort berry phase and pseudospin winding number in bilayer graphene
url http://hdl.handle.net/1721.1/69581
work_keys_str_mv AT marzarinicola berryphaseandpseudospinwindingnumberinbilayergraphene
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