max_ll_util.h.html | mathcode2html |
Source file: max_ll_util.h | |
Converted: Sat May 9 2015 at 14:44:17 | |
This documentation file will not reflect any later changes in the source file. |
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/* Copyright 2008-2011 Research Foundation State University of New York */ /* This file is part of QUB Express. */ /* QUB Express is free software; you can redistribute it and/or modify */ /* it under the terms of the GNU General Public License as published by */ /* the Free Software Foundation, either version 3 of the License, or */ /* (at your option) any later version. */ /* QUB Express is distributed in the hope that it will be useful, */ /* but WITHOUT ANY WARRANTY; without even the implied warranty of */ /* MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the */ /* GNU General Public License for more details. */ /* You should have received a copy of the GNU General Public License, */ /* named LICENSE.txt, in the QUB Express program directory. If not, see */ /* <http://www.gnu.org/licenses/>. */ #ifndef MAX_LL_UTIL_H #define MAX_LL_UTIL_H #include "ublas_plus.h" /*
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This unit provides common functions for MIL and MSL See also: Up: Index |
*/ /*
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The Q matrix of rate constants (probability per second) is computed from intrinsic rate constants K0 and K1, and potentially Ligand- and Voltage-sensitive. \[Q_{a,b} = K0_{a,b} * Ligand_{a,b} * e^{K1_{a,b} * Voltage_{a,b}}\] \[Q_{a,a} = - \sum_i Q_{a,i}\] |
*/ QUBFAST_API void BuildQ(int Ns, matrix<double>& Q, matrix<double>& K0, matrix<double>& K1, matrix<int>& Ligand, matrix<int>& Voltage, double *Constants); QUBFAST_API void BuildQ_p(int Ns, matrix<double>& Q, matrix<double>& K0, matrix<double>& K1, matrix<double>& K2, matrix<int>& Ligand, matrix<int>& Voltage, matrix<int>& Pressure, double *Constants); /*
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"Qe" aka \({}^eQ\) is the "apparent" rate constant matrix, given that events with duration <= tdead are not recorded. MIL and MSL compute the probability of staying in class a for duration t using the submatrix \({}^eQ_{aa}\) \[A(a, t) = e^{{}^eQ_{aa} t'}\] |
*/ QUBFAST_API void QtoQe(matrix<double>& Q, int *clazz, double tdead, matrix<double>& eQ); /*
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As discussed in (Milescu 2005), it can be preferable to start an experiment at equilibrium. Entry probabilities (P0) are then no longer constant, but a function of rate constants. We use the "direct" method given in Neher and Sakmann: Defining \(S = [Q | 1]\) and \(u\) a row vector of ones, \[P_{eq} = u \cdot (S \cdot S^T)^{-1}\] |
*/ QUBFAST_API void QtoPe(matrix<double>& Q, matrix<double>& Pe); /*
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As discussed in (Qin 1997), the forward probability vectors alpha must be frequently rescaled to 1 in order to stay within machine precision. Conveniently, the log likelihood is the sum of these log scaling factors. |
*/ QUBFAST_API double alpha_logscale(vector<double>& alpha); #endif