Monte Carlo prediction of ballistic effect on phonon transport in silicon in the presence of small localized heat source

材料科学 热流密度 声子 弹道传导 热导率 热传导 凝聚态物理 纳米计量学 蒙特卡罗方法 温度跃变 热阻 传热 纳米技术 机械 复合材料 光电子学 物理 电子 统计 数学 原子力显微镜 量子力学
作者
T. T. Trang Nghiêm,N. Trannoy,Jaona Randrianalisoa
出处
期刊:Nanotechnology [IOP Publishing]
卷期号:30 (41): 415403-415403 被引量:6
标识
DOI:10.1088/1361-6528/ab2c1c
摘要

Understanding phonon transport at nanoscale is critically important for thermal nanometrology applications including scanning thermal microscopy, three-omega and time domain thermoreflectance experiments. In this paper, a multidimensional non-gray Monte Carlo simulation is developed to investigate the ballistic phonon transport in a silicon sample heated on the top by a small localized heater line. We observed that heat confinement occurs for very small heat sources. This result contradicts the classical Fourier model, according to which the heat penetration depth is always significant, even with small sources. The temperature fields inside the sample exhibit different penetration depths depending strongly on the heater line size. Maximum thermal resistance and a large interface temperature jump take place in the limit of very small heater width compared to the phonon mean free path due to the nonequilibrium and ballistic nature of phonon transport. Increasing the heater width leads to a decrease in the heat flux and temperature jump. In the limit of a very large heat source, the heat flux and temperature jump become independent of heat source size. In accordance with experimental investigations for the case of sapphire material (Siemens et al 2010 Nature Mat. 9 26-30), the thermal resistance of the silicon sample due to the localized heat source decreases and then tends to reach a plateau with increasing source size from tens of nanometers to micrometers. These results are important, not only for understanding the thermal transport in the sample during nanometrology experiments, but also for the design and manipulation of heat at nanoscale.
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