Garfield++
v1r0
A toolkit for the detailed simulation of particle detectors based on ionisation measurement in gases and semiconductors
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chisran.h
Go to the documentation of this file.
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#ifndef CHISRAN_H
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#define CHISRAN_H
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#include "
wcpplib/safetl/AbsArr.h
"
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// Remake of CERN's subroutine hisran for generation of random numbers
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// according to histogram
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// I. B. Smirnov, 2003.
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// This is old programs.
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// The new ones are in wcpplib/math/tline.h
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// They are more generic, although the old ones should be working as well.
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float
chispre
(
float
*x,
float
*p,
float
*f,
long
q);
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// here x is a left side of interval on which
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// function p is a constant.
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// last point x[q] is the end of last interval.
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// p and f must have dimensions q.
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// x must have dimension q + 1
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// f is return array.
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// f[n] is normalized integral till the end of n'th interval or till
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// x[n+1].
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// Normalization is such that f[q-1]=1.0;
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// Return value is the true integral.
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float
chisran
(
float
flat_random_number,
float
*x,
float
*f,
long
q);
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double
chispre
(
DynLinArr<double>
&f,
int
s_allow_zero_f = 0);
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// here intervals are unit
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// function p is a constant along these intervals.
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// last point x[q] is the end of last interval.
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// p and f must have dimensions q.
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// f is return array.
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// f[n] is normalized integral till the end of n'th interval or till
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// x[n+1].
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// Normalization is such that f[q-1]=1.0;
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// Return value is the true integral.
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// Sun of f should be always more than zero.
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// if s_allow_zero_f = 1, some values of f are allowed to be
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// negative and they are made zero with diagnostic printed.
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// (this have sence only for debug.)
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double
chisran
(
double
flat_random_number,
DynLinArr<double>
f);
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#endif
AbsArr.h
chispre
float chispre(float *x, float *p, float *f, long q)
Definition:
chisran.cpp:7
chisran
float chisran(float flat_random_number, float *x, float *f, long q)
Definition:
chisran.cpp:22
DynLinArr
Definition:
AbsArr.h:156
garfieldpp-v1r0
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wcpplib
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chisran.h
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