Hall Drag and Magnetodrag in Graphene

Massless Dirac fermions in graphene at charge neutrality form a strongly interacting system in which both charged and neutral (energy) modes play an important role. These modes are essentially decoupled in the absence of a magnetic field, but become strongly coupled when the field is applied. We sho...

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Main Authors: Song, Justin Chien Wen, Levitov, Leonid
Other Authors: Massachusetts Institute of Technology. Department of Physics
Format: Article
Language:en_US
Published: American Physical Society 2014
Online Access:http://hdl.handle.net/1721.1/84980
https://orcid.org/0000-0002-4268-731X
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author Song, Justin Chien Wen
Levitov, Leonid
author2 Massachusetts Institute of Technology. Department of Physics
author_facet Massachusetts Institute of Technology. Department of Physics
Song, Justin Chien Wen
Levitov, Leonid
author_sort Song, Justin Chien Wen
collection MIT
description Massless Dirac fermions in graphene at charge neutrality form a strongly interacting system in which both charged and neutral (energy) modes play an important role. These modes are essentially decoupled in the absence of a magnetic field, but become strongly coupled when the field is applied. We show that this regime is characterized by strong magnetodrag and Hall drag, originating from long-range energy currents and spatial temperature gradients. The energy-driven effects arise in a wide temperature range, and feature an unusually strong dependence on field and carrier density. We argue that this mechanism accounts for the recently observed giant magnetodrag and Hall drag occurring at classically weak fields.
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spelling mit-1721.1/849802022-09-29T23:57:16Z Hall Drag and Magnetodrag in Graphene Song, Justin Chien Wen Levitov, Leonid Massachusetts Institute of Technology. Department of Physics Song, Justin Chien Wen Levitov, Leonid Massless Dirac fermions in graphene at charge neutrality form a strongly interacting system in which both charged and neutral (energy) modes play an important role. These modes are essentially decoupled in the absence of a magnetic field, but become strongly coupled when the field is applied. We show that this regime is characterized by strong magnetodrag and Hall drag, originating from long-range energy currents and spatial temperature gradients. The energy-driven effects arise in a wide temperature range, and feature an unusually strong dependence on field and carrier density. We argue that this mechanism accounts for the recently observed giant magnetodrag and Hall drag occurring at classically weak fields. 2014-02-18T17:25:09Z 2014-02-18T17:25:09Z 2013-09 2013-03 Article http://purl.org/eprint/type/JournalArticle 0031-9007 1079-7114 http://hdl.handle.net/1721.1/84980 Song, Justin C. W., and Leonid S. Levitov. “Hall Drag and Magnetodrag in Graphene.” Physical Review Letters 111, no. 12 (September 2013). © 2013 American Physical Society https://orcid.org/0000-0002-4268-731X en_US http://dx.doi.org/10.1103/PhysRevLett.111.126601 Physical Review Letters 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 American Physical Society
spellingShingle Song, Justin Chien Wen
Levitov, Leonid
Hall Drag and Magnetodrag in Graphene
title Hall Drag and Magnetodrag in Graphene
title_full Hall Drag and Magnetodrag in Graphene
title_fullStr Hall Drag and Magnetodrag in Graphene
title_full_unstemmed Hall Drag and Magnetodrag in Graphene
title_short Hall Drag and Magnetodrag in Graphene
title_sort hall drag and magnetodrag in graphene
url http://hdl.handle.net/1721.1/84980
https://orcid.org/0000-0002-4268-731X
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