Frequency-dependent Monte Carlo simulations of phonon transport in two-dimensional porous silicon with aligned pores
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Cites background from "Frequency-dependent Monte Carlo sim..."
...Anharmonic scattering is processed as a probabilistic step following the energy sampling [7]....
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...If interface scattering occurs, a random number is generated and compared with the relevant phonon’s transmissivity to determine whether transmission or reflection occurs subsequently [7]....
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Cites background or methods from "Frequency-dependent Monte Carlo sim..."
...es by V g;i t. The sampling substep during which the temperature (T) and pseudo-temperature (T loc) are locally measured. They are calculated by inverting the local energy (E) and pseudo-energy (E~) [10] relations E= N eff X i ~! i= V Z ! max !=0 X p D(!;p)~! exp ~! k bT 1 d! (7) and E~ = N eff X i ~! i ˝(! i;p i;T) = V Z ! max !=0 X p D(!;p)~! ˝(!;p;T) 1 exp ~! k bT loc 1 d! (8) respectively...
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...odic unit cell boundary conditions Heat transfer in periodic nanostructures is a subject of considerable interest in the context of many applications. Such nanostructures are considered in Hao et al. [10], in Huang et al. [21] and in Jeng et al. [4]. Hao et al. developed periodic boundary conditions that allow ecient simulation of such structures by considering only one unit cell (period). In this se...
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... method for eciently treating transmission and re ection of phonons at material interfaces and used this method to model the thermal conductivity of nanoparticle composites [4]. Hao et al. developed [10] a formulation for periodic boundary conditions in order to study the thermal conductivity of periodic nanoporous materials while only simulating one unit cell (period). The work presented here introd...
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...olution (56). Figure 4 shows a comparison between this solution and the variance-reduced Monte Carlo result. The simulation was run with T eq = T 0 and the phonon velocity was taken to be 12;360m:s 1 [10]. Excellent agreement is observed. 4.2 Heat ux and thermal conductivity in a thin slab In this section we continue to validate our formulation by calculating the thermal conductivity of a thin silicon...
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...lar by nature to a black body, have been used in several studies [8, 9]. Adiabatic boundaries also naturally appear [8, 20]. Recently, a class of periodic boundary conditions has also been introduced [10]. The deviational formulation adapts remarkably well to these dierent classes of boundary conditions. 3.5.1 Adiabatic boundaries Adiabatic boundaries re ect all incident phonons. This re ection proce...
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