Thermal van der Waals interaction between graphene layers

G. Gómez-Santos

Physical Review B · 2009 · 158 citations · 21 references

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TL;DR

The study examines the van der Waals interaction between two graphene sheets at finite temperatures. The force between graphene layers shows a crossover governed by the thermal length ξ_T, with a zero‑temperature regime for z≪ξ_T and a universal linear‑in‑T regime for z≫ξ_T, driven by classical plasmon behavior, while retardation is negligible and thermal effects become significant at tens of nanometers at room temperature.

Abstract

The van de Waals interaction between two graphene sheets is studied at finite temperatures. Graphene's thermal length $({\ensuremath{\xi}}_{T}=\ensuremath{\hbar}v/{k}_{B}T)$ controls the force versus distance $(z)$ as a crossover from the zero temperature results for $z⪡{\ensuremath{\xi}}_{T}$, to a linear-in-temperature, universal regime for $z⪢{\ensuremath{\xi}}_{T}$. The large separation regime is shown to be a consequence of the classical behavior of graphene's plasmons at finite temperature. Retardation effects are largely irrelevant, both in the zero and finite temperature regimes. Thermal effects should be noticeable in the van de Waals interaction already for distances of tens of nanometers at room temperature.

References

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