comfac

介绍matlab的gui使用，pdf格式(Introduction matlab gui, pdf format)

This is BOC AWGN Simulation zip file. It contains one folder(build setting) and 9 files(m file, mdl files etc..) Thank you

当线性代数联立方程组的系数矩阵为三对角阵T时，可将T分解为主对角元素为1的下三角阵L和另一个右三角阵R的积。(Simultaneous linear algebraic equations when the coefficient matrix is tridiagonal matrix T, can break down the main diagonal elements of T 1 of the lower triangular matrix L and the other right-triangular matrix R of the product.)

最新最全的SCI目录（大类加小类，齐全）(The newest polycysic SCI directory categories and subcategories complete )

One-Dimensional Discrete Wavelet Transforms (One-Dimensional Discrete Wavelet Transf orms)

newmark方法是实际应用程序，尤其适合初学者入门学习，易于消化。(Newmark method is a practical application, especially for beginners entry to learn, easy to digest.)

通過改變調製指數SDM和DDM的可以改變和測試通常使用在ILS (Instrument Landing 系統內)可以隨著改變SDM和DDM來看出它的種種特性 (Program to find SDM (Sum Depth of modulation)and DDM (Difference depth of modulation)Used in ILS (Instrument Landing System) Created by:Ashwini Deshpande, )

光子晶体的能带图计算，其实质就是电磁本征值（复矢量场）的问题。利用平面波展开磁场，引入f(r)=1/eps(r)，再利用倒格矢G将f(r)展开，将两者代入光子晶体的支配方程，最后得到一个平面波展开的方法的线性方程组，最终转化为求解其特征值向量的问题。(Energy band diagram of the photonic crystal, its essence is the electromagnetic eigenvalues ​ ​ (complex vector field).The linear plane wave expansion magnetic field, the introduction of f (r) = 1/eps (r), re-use reciprocal lattice vector G will expand f (r), the two substituted into the governing equations of the photonic crystal, and finally get a plane wave expansionequations, and ultimately into solving the problem of its eigenvalues​ ​ .)

功能强大、包含多种算法的小波分析工具箱，须在matlab下安装(A powerful, multi-algorithm of wavelet analysis toolbox, to be installed in the matlab)

A new method for periodic scattering problems using 2nd kind boundary integral equations and the free-space Green s function, adding extra degrees of freedom on the unit cell walls, and imposing quasi-periodicity in an expanded linear system.(A new method for periodic scattering problems using 2nd kind boundary integral equations and the free-space Green s function, adding extra degrees of freedom on the unit cell walls, and imposing quasi-periodicity in an expanded linear system. This avoids the problems with the standard approach, namely: the quasi-periodic Green s function is slow to evaluate, it diverges at Wood s anomalies, and it does not handle large aspect ratios well. Our new approach cures all three issues, and can easily be `wrapped around an existing code (e.g. fast-multipole acceleration) for the isolated-obstacle scattering problem. It includes the latest talk slides: "A new integral representation for quasi-periodic scattering problems in two dimensions")