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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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Efficient 2D k-Space Discretization and Non-Linear Interpolation Schemese denoted as ., ϕ. 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
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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
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Efficient 2D k-Space Discretization and Non-Linear Interpolation Schemessed on the coordinates ., ϕ has been used, which requires to solve the . ⋅. SE for many (., ϕ) 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
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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
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