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Refs #6670 added source and parameters for VISION
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Code/Mantid/Framework/Algorithms/inc/MantidAlgorithms/ModeratorTzero.h
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#ifndef MANTID_ALGORITHMS_MODERATORTZERO_H_ | ||
#define MANTID_ALGORITHMS_MODERATORTZERO_H_ | ||
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//---------------------------------------------------------------------- | ||
// Includes | ||
//---------------------------------------------------------------------- | ||
#include "MantidAPI/Algorithm.h" | ||
#include "MantidKernel/PhysicalConstants.h" | ||
#include "MantidGeometry/muParser_Silent.h" | ||
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namespace Mantid | ||
{ | ||
namespace Algorithms | ||
{ | ||
/* Corrects the time of flight (TOF) by a time offset that is dependent on the energy of the neutron after passing through the moderator. | ||
A heuristic formula for the correction is stored in the instrument definition file. Below is shown the entry in the instrument file for the VISION beamline: | ||
<!-- formula for t0 calculation. See http://muparser.sourceforge.net/mup_features.html#idDef2 for available operators--> | ||
<parameter name="t0_formula" type="string"> | ||
<value val="34.746 - 0.166672*incidentEnergy + 0.00020538*incidentEnergy^(2.0)" /> | ||
</parameter> | ||
The recorded TOF = t_0 + t_i + t_f with | ||
t_0: emission time from the moderator | ||
t_1: time from moderator to sample | ||
t_2: time from sample to detector | ||
This algorithm will replace TOF with TOF' = TOF-t_0 = t_i+t_f | ||
For a direct geometry instrument, the incidente energy E_1 is the same for all neutrons. Hence, the moderator emission time is the same for all neutrons. | ||
For an indirect geometry instrument, E_1 is different for each neutron and is not known. However, the final energy E_2 selected by the analyzers is known. | ||
t_0 = func(E_1) , a function of the incident energy | ||
t_1 = L_1/v_1 with L_1 the distance from moderator to sample, and v_1 the initial unknown velocity ( E_1=1/2*m*v_1^2) | ||
t_2 = L_2/v_2 with L_2 the distance from sample to detector, and v_2 is the final fixed velocity ( E_2=1/2*m*v_2^2) | ||
We obtain TOF' in an iterative process, taking into account the fact that the correction t_0 is much smaller than t_i+t_f. Thus | ||
TOF-t_0^(n) = L_1/v_1^(n) + L_2/v_2 , n=0, 1, 2,.. | ||
Set t_0^(0)=0 and obtain v_1^(0) from the previous formula. From v_1^(0) we obtain E_1^(0) | ||
Set t_0^(1)=func( E_1^(0) ) and repeat the steps until |t_0^(n+1) - t_0^(n+1)| < 1 microsec. Typically, three to four iterations are needed for convergence. | ||
@author Jose Borreguero | ||
@date 03/04/2013 | ||
Copyright © 2010 ISIS Rutherford Appleton Laboratory & NScD Oak Ridge National Laboratory | ||
This file is part of Mantid. | ||
Mantid 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. | ||
Mantid 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 | ||
along with this program. If not, see <http://www.gnu.org/licenses/>. | ||
File change history is stored at: <https://github.com/mantidproject/mantid> | ||
Code Documentation is available at: <http://doxygen.mantidproject.org> | ||
*/ | ||
class DLLExport ModeratorTzero : public Mantid::API::Algorithm | ||
{ | ||
public: | ||
/// (Empty) Constructor | ||
ModeratorTzero() : Mantid::API::Algorithm(), m_convfactor(0.5e+12*Mantid::PhysicalConstants::NeutronMass/Mantid::PhysicalConstants::meV), m_niter(1), m_t1min(200.0) {} | ||
/// Virtual destructor | ||
virtual ~ModeratorTzero() {} | ||
/// Algorithm's name | ||
virtual const std::string name() const { return "ModeratorTzero"; } | ||
/// Algorithm's version | ||
virtual int version() const { return (1); } | ||
/// Algorithm's category for identification | ||
virtual const std::string category() const { return "CorrectionFunctions\\InstrumentCorrections"; } | ||
/// set attribute m_formula | ||
void setFormula(const std::string &formula); | ||
/// output m_t1min | ||
double gett1min(); | ||
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private: | ||
Mantid::Geometry::Instrument_const_sptr m_instrument; | ||
/// Sets documentation strings for this algorithm | ||
virtual void initDocs(); | ||
// Initialisation code | ||
void init(); | ||
/// Execution code for histogram workspace | ||
void exec(); | ||
/// Execution code for event workspace | ||
void execEvent(); | ||
/// Calculate distance from source to sample or monitor | ||
double CalculateL1(Mantid::API::MatrixWorkspace_sptr inputWS, size_t i); | ||
/// Calculate time from sample to detector | ||
double CalculateT2(Mantid::API::MatrixWorkspace_sptr inputWS, size_t i); | ||
/// Calculate emission time from the moderator for a given detector (L1, t2) and TOF | ||
double CalculateT0(const double &tof, const double &L1, const double &t2, double &E1, mu::Parser &parser); | ||
const double m_convfactor; | ||
/// Maximum number of iterations when calculating the emission time from the moderator | ||
size_t m_niter; | ||
/// tolerance for calculating E1, in micro-seconds | ||
double m_tolTOF; | ||
/// string containing the heuristic regression for the moderator emission time versus neutron energy | ||
std::string m_formula; | ||
/// tof limit for fast neutrons | ||
const double m_t1min; | ||
}; | ||
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} // namespace Algorithms | ||
} // namespace Mantid | ||
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#endif /*MANTID_ALGORITHMS_MODERATORTZERO_H_*/ |
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