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Titlebook: Deterministic Solvers for the Boltzmann Transport Equation; Sung-Min Hong,Anh-Tuan Pham,Christoph Jungemann Book 2011 Springer-Verlag/Wien

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41#
發(fā)表于 2025-3-28 16:04:19 | 只看該作者
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發(fā)表于 2025-3-28 21:51:10 | 只看該作者
43#
發(fā)表于 2025-3-29 00:45:30 | 只看該作者
Efficient 2D k-Space Discretization and Non-Linear Interpolation Schemese denoted as .,??. The foci of this section are the efficient 2D .-space discretization and non-linear interpolation schemes. The . ?. solver consumes typically the largest part of the CPU time during transport simulations including the . ?. SE [1,?2,?3]. An efficient discretization of the 2D .-spac
44#
發(fā)表于 2025-3-29 04:47:15 | 只看該作者
45#
發(fā)表于 2025-3-29 11:15:23 | 只看該作者
Resultsng the simulation results to the long-channel low-field mobility measurements for bulk Si PMOSFETs from Takagi [5] at three lattice temperatures 223, 300, and 443?K shown in Fig.?12.1 (top). As in [3,?4], a phonon energy of .ω?=?61.?2?meV was used and kept fixed in this work. The other four scatteri
46#
發(fā)表于 2025-3-29 14:10:29 | 只看該作者
Efficient 2D k-Space Discretization and Non-Linear Interpolation Schemessed on the coordinates .,?? has been used, which requires to solve the . ?. SE for many (.,??) grid points in order to get an accurate energy interpolation. In this work, the subband energy and the probability density function for an arbitrary in-plane wave vector are determined by an efficient inte
47#
發(fā)表于 2025-3-29 19:06:55 | 只看該作者
Iteration Methodsht)) with the new deterministic method to solve BTE converge linearly with simulation time similar to the Gummel loop in the classical drift-diffusion based TCAD device simulators [4,?6], and thus much faster than an MC algorithm with its square root dependence?[7]. In addition, the deterministic re
48#
發(fā)表于 2025-3-29 23:29:41 | 只看該作者
49#
發(fā)表于 2025-3-30 02:04:26 | 只看該作者
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發(fā)表于 2025-3-30 05:40:34 | 只看該作者
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