GIANT INTRINSIC CARRIER MOBILITIES IN GRAPHENE AND ITS BILAYER PDF

Phys Rev Lett. Jan 11;(1) Epub Jan 7. Giant intrinsic carrier mobilities in graphene and its bilayer. Morozov SV(1), Novoselov KS. Giant Intrinsic Carrier Mobilities in Graphene and Its Bilayer. S. V. Morozov,1,2 K. S. Novoselov,1 M. I. Katsnelson,3 F. Schedin,1 D. C. Elias,1. Abstract. We have studied temperature dependences of electron transport in graphene and its bilayer and found extremely low.

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Publisher’s version of record: Physical Review Letters, 1. Skip to main content. Publication Title Physical Review Letters. Sign up to receive bi,ayer email alerts from Physical Review Letters. MorozovUniversity of Manchester K.

A sharp thresholdlike increase in resistivity observed above similar to K is unexpected but can qualitatively be understood within a model of a rippled graphene sheet in which scattering occurs on intraripple flexural phonons. We have studied temperature dependences of electron transport in graphene and its bilayer and found extremely low electron-phonon scattering rates that set the fundamental limit on possible charge carrier mobilities at room temperature.

Series I Physics Physique Fizika. Weyl fermions are observed in a solid. Abstract We have studied temperature dependences of electron transport in graphene and its bilayer and found extremely grzphene electron-phonon scattering rates that set the fundamental limit on possible charge carrier mobilities at room temperature.

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KatsnelsonUniversity of Nijmegen F. Bibliographic metadata Type of resource:.

Recommended Citation Morozov, S. We have studied temperature dependences of electron transport in graphene and its bilayer and found extremely low electron-phonon scattering rates that set the fundamental limit on possible charge carrier mobilities at room temperature. EliasUniversity of Manchester John A. Elias 1J. SchedinUniversity of Manchester D. Figure 4 T dependence in bilayer graphene.

[] Giant Intrinsic Carrier Mobilities in Graphene and Its Bilayer

Related resources Full-text held externally DOI: Department of Physics Publications. Record metadata Manchester eScholar ID:. We have studied temperature dependences of electron transport in graphene and its bilayer and found extremely low electron-phonon scattering rates that set the fundamental limit on possible charge carrier mobilities at room goant.

The experiments were carried out in a field of 0. Abstract We have studied temperature dependences of electron transport in graphene and its bilayer and found extremely low electron-phonon scattering rates that set the fundamental limit on possible charge carrier intrinsi at room temperature.

Figure 3 T -dependent part of resistivity for 4 SLG samples symbols.

Giant intrinsic carrier mobilities in graphene and its bilayer.

NovoselovUniversity of Manchester M. Library subscriptions will be modified accordingly. University researcher s Konstantin Novoselov’s research staff profile. Jaszczak 4and A. GeimUniversity of Manchester.

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Giant intrinsic carrier mobilities inhrinsic graphene and its bilayer. Institutional metadata University researcher s:. Schedin 1D. To view the content in your browser, please download Adobe Reader or, alternately, you may Download the file to your hard drive.

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Giant intrinsic carrier mobilities in graphene and its bilayer.

Abstract We have studied temperature dependences of electron transport in graphene and its bilayer and found extremely low electron-phonon scattering rates that set the fundamental limit mobilihies possible charge carrier mobilities inttinsic room temperature. Katsnelson 3F. This arrangement will initially last for two years, up to the end of Included in Physics Commons.

The solid curve is the best fit by using a combination bilauer T and T 5 functions, which serves here as a guide to the eye. Title Giant intrinsic carrier mobilities in graphene and its bilayer. The library chat service will be available from 11am-3pm Monday to Friday excluding Bank Holidays. Morozov 1,2K.

Giant intrinsic carrier mobilities in graphene and its bilayer. Novoselov 1M.