TY  - JOUR
AU  - Jaćimovski, Stevo
AU  - Bukurov, Masa
AU  - Šetrajčić, Jovan P.
AU  - Raković, Dejan
PY  - 2015
UR  - http://jakov.kpu.edu.rs/handle/123456789/638
AB  - The study of graphene thermal conductivity is of great importance, as its anomalous thermal and electrical conductivities (the largest among the all known materials so far) provide very good perspectives for graphene-based nanoelectronics devices. Thermal conductivity of graphene is phonon-based, since its electronic-based thermal conductivity represents less than 1% of the total thermal conductivity at room temperature. For the consideration of the thermal conductivity of graphene the Boltzmann equation in the approximation of relaxation time is used. The relaxation time is determined, with three mechanisms of phonon scattering accounted simultaneously: at defects, at borders, and on phonons. Temperature dependence of thermal conductivity is determined numerically in the range from 15 K to 400 K. The results obtained are in accordance with some other available results found in literature, obtained either experimentally or by numerical calculations.
PB  - Academic Press Ltd- Elsevier Science Ltd, London
T2  - Superlattices and microstructures
T1  - Phonon thermal conductivity of graphene
VL  - 88
SP  - 330
EP  - 337
DO  - 10.1016/j.spmi.2015.09.027
ER  - 

@article{
author = "Jaćimovski, Stevo and Bukurov, Masa and Šetrajčić, Jovan P. and Raković, Dejan",
year = "2015",
abstract = "The study of graphene thermal conductivity is of great importance, as its anomalous thermal and electrical conductivities (the largest among the all known materials so far) provide very good perspectives for graphene-based nanoelectronics devices. Thermal conductivity of graphene is phonon-based, since its electronic-based thermal conductivity represents less than 1% of the total thermal conductivity at room temperature. For the consideration of the thermal conductivity of graphene the Boltzmann equation in the approximation of relaxation time is used. The relaxation time is determined, with three mechanisms of phonon scattering accounted simultaneously: at defects, at borders, and on phonons. Temperature dependence of thermal conductivity is determined numerically in the range from 15 K to 400 K. The results obtained are in accordance with some other available results found in literature, obtained either experimentally or by numerical calculations.",
publisher = "Academic Press Ltd- Elsevier Science Ltd, London",
journal = "Superlattices and microstructures",
title = "Phonon thermal conductivity of graphene",
volume = "88",
pages = "330-337",
doi = "10.1016/j.spmi.2015.09.027"
}

Jaćimovski, S., Bukurov, M., Šetrajčić, J. P.,& Raković, D.. (2015). Phonon thermal conductivity of graphene. in Superlattices and microstructures
Academic Press Ltd- Elsevier Science Ltd, London., 88, 330-337.
https://doi.org/10.1016/j.spmi.2015.09.027

Jaćimovski S, Bukurov M, Šetrajčić JP, Raković D. Phonon thermal conductivity of graphene. in Superlattices and microstructures. 2015;88:330-337.
doi:10.1016/j.spmi.2015.09.027 .

Jaćimovski, Stevo, Bukurov, Masa, Šetrajčić, Jovan P., Raković, Dejan, "Phonon thermal conductivity of graphene" in Superlattices and microstructures, 88 (2015):330-337,
https://doi.org/10.1016/j.spmi.2015.09.027 . .