TY - JOUR
T1 - Lattice thermal conductivity of penta-graphene
AU - Wang, Fancy Qian
AU - Yu, Jiabing
AU - Wang, Qian
AU - Kawazoe, Yoshiyuki
AU - Jena, Puru
N1 - Funding Information:
This work is partially supported by grants from the National Natural Science Foundation of China ( NSFC-51471004 ), the National Grand Fundamental Research 973 Program of China (Grant 2012CB921404 ), and the Doctoral Program of Higher Education of China ( 20130001110033 ). P.J. acknowledges support by the U.S. Department of Energy , Office of Basic Energy Sciences, Division of Materials Sciences and Engineering under Award #DE-FG02-96ER45579 . Y.K. would like to thank ONR Global and ITC-PAC for the support by the Grant No. N62909-16-1-2036 . The authors thank the crew of the Center for Computational Materials Science, the Institute for Materials Research, Tohoku University (Japan), for their continuous support of the HITACHI SR11000 supercomputing facility.
Publisher Copyright:
© 2016 Elsevier Ltd. All rights reserved.
PY - 2016/8/1
Y1 - 2016/8/1
N2 - Motivated by the unique geometry and novel properties of penta-graphene proposed recently as a new carbon allotrope consisting of pure pentagons [Zhang et al. Proc. Natl. Acad. Sci. 2015, 112, 2372], we systematically investigated its phonon transport properties by solving exactly the linearized phonon Boltzmann transport equation combined with first principles calculations. The intrinsic lattice thermal conductivity Klat of penta-graphene is found to be about 645 W/mK at room temperature, which is significantly reduced as compared to that of graphene. The underlying reason is the strong anharmonic effect introduced by the buckled pentagonal structure with hybridized sp2 and sp3 bonding. A detailed analysis of the phonons of penta-graphene reveals that the ZA mode is the primary heat carrier (nearly 60%). The Klat is dominated by three-phonon scattering where the scattering rate of the Normal scattering process is comparable to that of the Umklapp scattering process. The phonon mean free path of the collective phonon excitations is in the order of micrometers. Complementing the high thermal conductivity of graphene, the low thermal conductivity of penta-graphene adds additional features to the family of carbon materials for thermal applications.
AB - Motivated by the unique geometry and novel properties of penta-graphene proposed recently as a new carbon allotrope consisting of pure pentagons [Zhang et al. Proc. Natl. Acad. Sci. 2015, 112, 2372], we systematically investigated its phonon transport properties by solving exactly the linearized phonon Boltzmann transport equation combined with first principles calculations. The intrinsic lattice thermal conductivity Klat of penta-graphene is found to be about 645 W/mK at room temperature, which is significantly reduced as compared to that of graphene. The underlying reason is the strong anharmonic effect introduced by the buckled pentagonal structure with hybridized sp2 and sp3 bonding. A detailed analysis of the phonons of penta-graphene reveals that the ZA mode is the primary heat carrier (nearly 60%). The Klat is dominated by three-phonon scattering where the scattering rate of the Normal scattering process is comparable to that of the Umklapp scattering process. The phonon mean free path of the collective phonon excitations is in the order of micrometers. Complementing the high thermal conductivity of graphene, the low thermal conductivity of penta-graphene adds additional features to the family of carbon materials for thermal applications.
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U2 - 10.1016/j.carbon.2016.04.054
DO - 10.1016/j.carbon.2016.04.054
M3 - Article
AN - SCOPUS:84965105737
SN - 0008-6223
VL - 105
SP - 424
EP - 429
JO - Carbon
JF - Carbon
ER -