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function G = lpcgain(xi,P) % lpcgain --> Gain estimation from prediction error energy. % % % G = lpcgain(xi,P) % % % The gain across speech frames, returned in vector

The routines use a common data structure 'hmm' with fields: hmm.train.cyc max number of cycles through data .tol termination tolerance of likelihood .rdisplay continous output of free energy

/* Copyright (c) 2003, The Regents of the University of California, through Lawrence Berkeley National Laboratory (subject to receipt of any required approvals from the U.S. Dept. of Energy). All rig

/* -4/20/2006: Petre M. -this file contains definitions that characterize the energy meter */ //this is the larger display #define GOWORLD_LCD #define LCD_5V //this is the number of digit

package org.openscience.cdk.modeling.forcefield; import javax.vecmath.GMatrix; import javax.vecmath.GVector; /** * Interface for a potential energy function to optimise in cdk/modeling/forcefield

List of errata and changes in version 2 of suboptimal folding code. 1. This small bug would give an energy of zero to a hairpin loop of size 3 when the closing base pa

afterburner2 { High-energy electron bunch enters a quiet plasma in cylindrical geometry -- Modeling the SLAC "afterburner" concept of Tom Katsouleas. This input file includes the effects of electron

afterburner4 { High-energy electron bunch enters a quiet plasma in cylindrical geometry -- Modeling the SLAC "afterburner" concept of Tom Katsouleas. This input file includes the effects of electron

afterburner3 { High-energy electron bunch enters a quiet plasma in cylindrical geometry -- Modeling the SLAC "afterburner" concept of Tom Katsouleas. This input file includes the effects of electron

afterburner { High-energy electron bunch enters a quiet plasma in cylindrical geometry -- Modeling the SLAC "afterburner" concept of Tom Katsouleas. This input file IGNORES the effects of electron-i