Heat conduction below diffusive limit in amorphous superlattice structures

被引:13
作者
Liao, Yuxuan [1 ]
Iwamoto, Sotaro [1 ]
Sasaki, Michiko [2 ]
Goto, Masahiro [2 ]
Shiomi, Junichiro [1 ,2 ]
机构
[1] Univ Tokyo, Dept Mech Engn, Bunkyo Ku, 7-3-1 Hongo, Tokyo 1138656, Japan
[2] Natl Inst Mat Sci, Ctr Mat Res Informat Integrat, 1-2-1 Sengen, Tsukuba, Ibaraki 3050047, Japan
基金
日本学术振兴会; 日本科学技术振兴机构;
关键词
Amorphous superlattice; Diffuson transport; Ballistic transport; Silicon and silica; Thermoreflectance; BOLTZMANN TRANSPORT-EQUATION; THERMAL-CONDUCTIVITY; VIBRATIONS; PHONONS; SOLVER;
D O I
10.1016/j.nanoen.2021.105903
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
Advanced means to further reduce the thermal conductivity of dense amorphous materials by nanostructuring is important for thermal management in future electronic and optical devices. While the works so far have realized the reduction by scattering propagons, here, we demonstrate that nanostructures can in addition inhibit transport of diffusons, by measuring the thermal conductivity of amorphous-silicon/amorphous-silica superlattices with a periodicity ranging from 4.5 nm to 29.3 nm at room temperature. The measurements show that thermal conductivity of the superlattice with periodicity below 9.5 nm is significantly below the amorphous diffusive limit (similar to 1 W/m K). The measured thermal conductivity can be reproduced using a combination of the phonon-gas kinetics model and Allen-Feldmann theory without any fitting parameters, with the interfacial transmittance of propagons and diffusons obtained by atomistic Green's function. In addition to the known reduction of propagon transport, the effective mean free paths of diffusons are reduced from that of the bulk (1-3 nm) to several angstroms or even atomistic by extreme boundary scattering at the interfaces in the superlattice, giving rise to a significant tunability of the amorphous thermal conductivity using truly nanoscale structures. The influence of interface scattering on the diffusion transport can be effectively described by the Boltzmann transport equation, and in this sense, propagons and diffusons do not fundamentally differ. Data and materials availability: All data needed to evaluate the conclusions in the paper are present in the and/or the Supplementary Materials. Additional data related to this paper may be requested from the authors.
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页数:6
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