Theory of substrate-directed heat dissipation for single-layer graphene and other two-dimensional crystals
arXiv:1608.00516 · doi:10.1103/PhysRevB.94.165427
Abstract
We present a theory of the phononic thermal (Kapitza) resistance at the interface between graphene or another single-layer two-dimensional (2D) crystal (e.g. MoS) and a flat substrate, based on a modified version of the cross-plane heat transfer model by Persson, Volokitin and Ueba [J. Phys.: Condens. Matter 23, 045009 (2011)]. We show how intrinsic flexural phonon damping is necessary for obtaining a finite Kapitza resistance and also generalize the theory to encased single-layer 2D crystals with a superstrate. We illustrate our model by computing the thermal boundary conductance (TBC) for bare and SiO-encased single-layer graphene and MoS on a SiO substrate, using input parameters from first-principles calculation. The estimated room temperature TBC for bare (encased) graphene and MoS on SiO are 34.6 (105) and 3.10 (5.07) MWKm, respectively. The theory predicts the existence of a phonon frequency crossover point, below which the low-frequency flexural phonons in the bare 2D crystal do not dissipate energy efficiently to the substrate. We explain within the framework of our theory how the encasement of graphene with a top SiO layer introduces new low-frequency transmission channels which significantly reduce the graphene-substrate Kapitza resistance. We emphasize that the distinction between bare and encased 2D crystals must be made in the analysis of cross-plane heat dissipation to the substrate.
arXiv comment12 pages, 8 figures
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Cited by in corpus (13)
- Energy Dissipation in Monolayer MoS Electronics
- Thermal Boundary Conductance of Two-Dimensional Interfaces
- Thickness-dependent Kapitza resistance in multilayered graphene and other two-dimensional crystals
- Spatiotemporal Mapping of Photocurrent in a Monolayer Semiconductor Using a Diamond Quantum Sensor
- Contribution of the acoustic waves to near-field heat transfer
- Electric double layer effect in an extreme near-field heat transfer between metal surfaces
- Electric field effect in heat transfer in 2D devices
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