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Finite-temperature Casimir effect for graphene. / Fialkovsky, Ignat V.; Marachevsky, Valery N.; Vassilevich, Dmitri V.

в: Physical Review B - Condensed Matter and Materials Physics, Том 84, № 3, 035446, 28.07.2011.

Результаты исследований: Научные публикации в периодических изданиях › статья › Рецензирование

Harvard

Fialkovsky, IV, Marachevsky, VN & Vassilevich, DV 2011, 'Finite-temperature Casimir effect for graphene', Physical Review B - Condensed Matter and Materials Physics, Том. 84, № 3, 035446. https://doi.org/10.1103/PhysRevB.84.035446, https://doi.org/10.1103/PhysRevB.84.035446

APA

Fialkovsky, I. V., Marachevsky, V. N., & Vassilevich, D. V. (2011). Finite-temperature Casimir effect for graphene. Physical Review B - Condensed Matter and Materials Physics, 84(3), [035446]. https://doi.org/10.1103/PhysRevB.84.035446, https://doi.org/10.1103/PhysRevB.84.035446

Vancouver

Fialkovsky IV, Marachevsky VN, Vassilevich DV. Finite-temperature Casimir effect for graphene. Physical Review B - Condensed Matter and Materials Physics. 2011 Июль 28;84(3). 035446. https://doi.org/10.1103/PhysRevB.84.035446, https://doi.org/10.1103/PhysRevB.84.035446

Author

Fialkovsky, Ignat V. ; Marachevsky, Valery N. ; Vassilevich, Dmitri V. / Finite-temperature Casimir effect for graphene. в: Physical Review B - Condensed Matter and Materials Physics. 2011 ; Том 84, № 3.

BibTeX

@article{db2b16b1515d4ad993ff376a7d124601,
title = "Finite-temperature Casimir effect for graphene",
abstract = "We adopt the Dirac model for quasiparticles in graphene and calculate the finite-temperature Casimir interaction between a suspended graphene layer and a parallel conducting surface. We find that at high temperature, the Casimir interaction in such system is just one-half of that for two ideal conductors separated by the same distance. In this limit, a single graphene layer behaves exactly as a Drude metal. In particular, the contribution of the TE mode is suppressed, while the contribution of the TM mode saturates at the ideal-metal value. The behavior of the Casimir interaction for intermediate temperatures and separations accessible in experiments is studied in some detail. We also find an interesting interplay between two fundamental constants of graphene physics: the fine-structure constant and the Fermi velocity.",
keywords = "FORCE, DENSITY, RANGE",
author = "Fialkovsky, {Ignat V.} and Marachevsky, {Valery N.} and Vassilevich, {Dmitri V.}",
year = "2011",
month = jul,
day = "28",
doi = "10.1103/PhysRevB.84.035446",
language = "Английский",
volume = "84",
journal = "Physical Review B-Condensed Matter",
issn = "1098-0121",
publisher = "American Physical Society",
number = "3",

}

RIS

TY - JOUR

T1 - Finite-temperature Casimir effect for graphene

AU - Fialkovsky, Ignat V.

AU - Marachevsky, Valery N.

AU - Vassilevich, Dmitri V.

PY - 2011/7/28

Y1 - 2011/7/28

N2 - We adopt the Dirac model for quasiparticles in graphene and calculate the finite-temperature Casimir interaction between a suspended graphene layer and a parallel conducting surface. We find that at high temperature, the Casimir interaction in such system is just one-half of that for two ideal conductors separated by the same distance. In this limit, a single graphene layer behaves exactly as a Drude metal. In particular, the contribution of the TE mode is suppressed, while the contribution of the TM mode saturates at the ideal-metal value. The behavior of the Casimir interaction for intermediate temperatures and separations accessible in experiments is studied in some detail. We also find an interesting interplay between two fundamental constants of graphene physics: the fine-structure constant and the Fermi velocity.

AB - We adopt the Dirac model for quasiparticles in graphene and calculate the finite-temperature Casimir interaction between a suspended graphene layer and a parallel conducting surface. We find that at high temperature, the Casimir interaction in such system is just one-half of that for two ideal conductors separated by the same distance. In this limit, a single graphene layer behaves exactly as a Drude metal. In particular, the contribution of the TE mode is suppressed, while the contribution of the TM mode saturates at the ideal-metal value. The behavior of the Casimir interaction for intermediate temperatures and separations accessible in experiments is studied in some detail. We also find an interesting interplay between two fundamental constants of graphene physics: the fine-structure constant and the Fermi velocity.

KW - FORCE

KW - DENSITY

KW - RANGE

U2 - 10.1103/PhysRevB.84.035446

DO - 10.1103/PhysRevB.84.035446

M3 - статья

VL - 84

JO - Physical Review B-Condensed Matter

JF - Physical Review B-Condensed Matter

SN - 1098-0121

IS - 3

M1 - 035446

ER -

ID: 5142338