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/*************************************************************************** * * VOICIN Version 52 * *************************************************************************** * * Voi

function [W,A]=desa2(x, dt) % The function DESA2 calculates frequency and amplitude using Teager Energy Operator (DESA-2 algorithm) % of the data x(n,m), where n is the number of points, and m is

function [W,A]=desa1(x, dt) % The function DESA1 calculates frequency and amplitude using Teager Energy Operator (DESA-1 algorithm) % for the data x(n,m), where n is the number of points, and m is

function [W,A]=desa(x, dt) % The function DESA calculates frequency and amplitude using Teager Energy Operator % for the data x(n,m), where n is the number of points, and m is % the number of

/********************************************************************** Each of the companies; Lucent, Motorola, Nokia, and Qualcomm (hereinafter referred to individually as "Source" or collectivel

%> solves for the eigenvalues of a rectangular, infinitely %> deep well in 2D, of variable area and ratio. It calculates the %> spectrum and the spectrum of energy differences. %> Variable

function f=numerov1(x0,x1,N,P,mult,E,Y0,DY0); %> The file integrates the 1D Schrodinger equation %> for an 'arbitrary' potential using the Numerov method. %> It produces the function val

/* satest2.c++ Simple experiments with simulated annealing find the nonlinear least squares optimum solution usage: satest2 input.file */ static const char rcsid[] = "@(#)satest2.c

% % FUNCTION 2.5 : "cp0201_waveform" % % Generates the energy-normalized pulse waveform % % Special case of the second derivative Gaussian pulse: % SCHOLTZ'S MONOCYCLE % % ********************

/* satest2.c++ Simple experiments with simulated annealing find the nonlinear least squares optimum solution usage: satest2 input.file */ static const char rcsid[] = "@(#)satest2.c