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Thermometry for Dirac fermions in graphene

We use both the zero-magnetic-field resistivity and the phase coherence time determined by weak localization as independent thermometers for Dirac fermions (DF) in multilayer graphene. In the high current (I) region, there exists a simple power law T DF ∝ I ~0.5 , where T DF is the effective Dirac f...

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Published in:Journal of the Korean Physical Society 2015, 66(1), , pp.1-6
Main Authors: Liu, Fan-Hung, Hsu, Chang-Shun, Lo, Shun-Tsung, Chuang, Chiashain, Huang, Lung-I, Woo, Tak-Pong, Liang, Chi-Te, Fukuyama, Y., Yang, Y., Elmquist, R. E., Wang, Pengjie, Lin, Xi
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cited_by cdi_FETCH-LOGICAL-c334t-534251a7c08c7fc46c370652b8e56f54cfef3962b3cbffba6e8ed200e07028d13
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container_title Journal of the Korean Physical Society
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creator Liu, Fan-Hung
Hsu, Chang-Shun
Lo, Shun-Tsung
Chuang, Chiashain
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Yang, Y.
Elmquist, R. E.
Wang, Pengjie
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description We use both the zero-magnetic-field resistivity and the phase coherence time determined by weak localization as independent thermometers for Dirac fermions (DF) in multilayer graphene. In the high current (I) region, there exists a simple power law T DF ∝ I ~0.5 , where T DF is the effective Dirac fermion temperature for epitaxial graphene on SiC. In contrast, T DF ∝ I ~1 in exfoliated multilayer graphene. We discuss possible reasons for the different power laws observed in these multilayer graphene systems. Our experimental results on DF-phonon scattering may find applications in graphene-based nanoelectronics.
doi_str_mv 10.3938/jkps.66.1
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subjects Mathematical and Computational Physics
Particle and Nuclear Physics
Physics
Physics and Astronomy
Theoretical
물리학
title Thermometry for Dirac fermions in graphene
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