- Extended the usage of xml-startup files in some plugin libraries and renamed the file itself.
- Added some documentation to libLFRelaxation which in the present stage is mainly used for testing purposes.
This commit is contained in:
Bastian M. Wojek
194
src/external/libLFRelaxation/TLFRelaxation.h
vendored
194
src/external/libLFRelaxation/TLFRelaxation.h
vendored
@ -5,7 +5,7 @@
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Author: Bastian M. Wojek
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e-mail: bastian.wojek@psi.ch
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2008/12/04
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$Id$
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***************************************************************************/
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@ -35,6 +35,7 @@
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#include<vector>
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#include<cstdio>
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#include<cmath>
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#include<map>
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using namespace std;
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@ -50,6 +51,15 @@ using namespace std;
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#include "fftw3.h"
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#include "../BMWIntegrator/BMWIntegrator.h"
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//-----------------------------------------------------------------------------------------------------------------
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/**
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* <p>User function for a static Gaussian depolarization in a longitudinal field using direct integration through GSL
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* See also: R. S. Hayano, Y. J. Uemura, J. Imazato, N. Nishida, T. Yamazaki, and R. Kubo,
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* \htmlonly Phys. Rev. B <b>20</b>, 850–859 (1979), doi:<a href="http://dx.doi.org/10.1103/PhysRevB.20.850">10.1103/PhysRevB.20.850</a>
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* \endhtmlonly
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* \latexonly Phys. Rev. B \textbf{20}, 850--859 (1979), \texttt{http://dx.doi.org/10.1103/PhysRevB.20.850}
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* \endlatexonly
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*/
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class TLFStatGssKT : public PUserFcnBase {
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public:
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@ -63,16 +73,29 @@ public:
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double operator()(double, const vector<double>&) const;
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private:
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TIntSinGss *fIntSinGss;
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TIntSinGss *fIntSinGss; ///< integrator
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mutable map<double, double> fIntValues; ///< previously calculated integral values
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mutable vector<double> fPar; ///< parameters of the function [\htmlonly ν<sub>L</sub>=<i>B</i>γ<sub>μ</sub>/2π (MHz), σ (μs<sup>-1</sup>)\endhtmlonly \latexonly $\nu_{\mathrm{L}}=B\gamma_{\mu}/2\pi~(\mathrm{MHz})$, $\sigma~(\mu\mathrm{s}^{-1})$ \endlatexonly]
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mutable bool fCalcNeeded; ///< flag specifying if an integration has to be done
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mutable double fLastTime; ///< time of the last calculated function value
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ClassDef(TLFStatGssKT,1)
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ClassDef(TLFStatGssKT,2)
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};
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class TLFStatLorKT : public PUserFcnBase {
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//-----------------------------------------------------------------------------------------------------------------
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/**
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* <p>User function for a static exponential depolarization in a longitudinal field using direct integration through GSL
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* See also: Y. J. Uemura, T. Yamazaki, D. R. Harshman, M. Senba, and E. J. Ansaldo,
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* \htmlonly Phys. Rev. B <b>31</b>, 546–563 (1985), doi:<a href="http://dx.doi.org/10.1103/PhysRevB.31.546">10.1103/PhysRevB.31.546</a>
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* \endhtmlonly
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* \latexonly Phys. Rev. B \textbf{31}, 546--563 (1985), \texttt{http://dx.doi.org/10.1103/PhysRevB.31.546}
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* \endlatexonly
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*/
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class TLFStatExpKT : public PUserFcnBase {
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public:
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TLFStatLorKT();
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~TLFStatLorKT();
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TLFStatExpKT();
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~TLFStatExpKT();
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Bool_t NeedGlobalPart() const { return false; }
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void SetGlobalPart(vector<void *> &globalPart, UInt_t idx) { }
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@ -81,11 +104,31 @@ public:
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double operator()(double, const vector<double>&) const;
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private:
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TIntBesselJ0Exp *fIntBesselJ0Exp;
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TIntBesselJ0Exp *fIntBesselJ0Exp; ///< integrator
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mutable map<double, double> fIntValues; ///< previously calculated integral values
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mutable vector<double> fPar; ///< parameters of the function [\htmlonly ν<sub>L</sub>=<i>B</i>γ<sub>μ</sub>/2π (MHz), <i>a</i> (μs<sup>-1</sup>)\endhtmlonly \latexonly $\nu_{\mathrm{L}}=B\gamma_{\mu}/2\pi~(\mathrm{MHz})$, $a~(\mu\mathrm{s}^{-1})$ \endlatexonly]
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mutable bool fCalcNeeded; ///< flag specifying if an integration has to be done
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mutable double fLastTime; ///< time of the last calculated function value
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ClassDef(TLFStatLorKT,1)
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ClassDef(TLFStatExpKT,2)
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};
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//-----------------------------------------------------------------------------------------------------------------
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/**
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* <p>User function for a dynamic Gaussian depolarization in a longitudinal field calculated using Laplace transforms
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* See also: R. S. Hayano, Y. J. Uemura, J. Imazato, N. Nishida, T. Yamazaki, and R. Kubo,
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* \htmlonly Phys. Rev. B <b>20</b>, 850–859 (1979), doi:<a href="http://dx.doi.org/10.1103/PhysRevB.20.850">10.1103/PhysRevB.20.850</a>
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* \endhtmlonly
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* \latexonly Phys. Rev. B \textbf{20}, 850--859 (1979), \texttt{http://dx.doi.org/10.1103/PhysRevB.20.850}
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* \endlatexonly
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*
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* For details regarding the numerical Laplace transform, see e.g.
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* P. Moreno and A. Ramirez,
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* \htmlonly IEEE Trans. Power Delivery <b>23</b>, 2599–2609 (2008), doi:<a href="http://dx.doi.org/10.1109/TPWRD.2008.923404">10.1109/TPWRD.2008.923404</a>
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* \endhtmlonly
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* \latexonly IEEE Trans. Power Delivery \textbf{23}, 2599--2609 (2008), \texttt{http://dx.doi.org/10.1109/TPWRD.2008.923404}
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* \endlatexonly
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*/
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class TLFDynGssKT : public PUserFcnBase {
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public:
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@ -99,28 +142,51 @@ public:
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double operator()(double, const vector<double>&) const;
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private:
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mutable vector<double> fPar;
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mutable bool fCalcNeeded;
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mutable bool fFirstCall;
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string fWisdom;
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unsigned int fNSteps;
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double fDt;
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double fDw;
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double fC;
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fftwf_plan fFFTplanFORW;
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fftwf_plan fFFTplanBACK;
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float *fFFTtime;
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fftwf_complex *fFFTfreq;
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mutable unsigned int fCounter;
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mutable vector<double> fPar; ///< parameters of the function [\htmlonly ν<sub>L</sub>=<i>B</i>γ<sub>μ</sub>/2π (MHz), σ (μs<sup>-1</sup>), ν (MHz)\endhtmlonly \latexonly $\nu_{\mathrm{L}}=B\gamma_{\mu}/2\pi~(\mathrm{MHz})$, $\sigma~(\mu\mathrm{s}^{-1})$, $\nu~(\mathrm{MHz})$ \endlatexonly]
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mutable bool fCalcNeeded; ///< flag indicating if the expensive Laplace transform has to be done (e.g. after parameters have changed)
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mutable bool fFirstCall; ///< flag indicating if the function is evaluated for the first time
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bool fUseWisdom; ///< flag showing if a FFTW3-wisdom file is used
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string fWisdom; ///< path to the wisdom file
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unsigned int fNSteps; ///< length of the Laplace transform
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double fDt; ///< time resolution
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double fDw; ///< frequency resolution
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double fC; ///< coefficient depending on the length of the Laplace transform and time resolution
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fftwf_plan fFFTplanFORW; ///< FFTW3 plan: time domain \htmlonly → \endhtmlonly \latexonly $\rightarrow$ \endlatexonly frequency domain
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fftwf_plan fFFTplanBACK; ///< FFTW3 plan: time domain \htmlonly ← \endhtmlonly \latexonly $\leftarrow$ \endlatexonly frequency domain
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float *fFFTtime; ///< time-domain array
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fftwf_complex *fFFTfreq; ///< frequency-domain array
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mutable unsigned int fCounter; ///< counter determining how many Laplace transforms are done (mainly for debugging purposes)
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ClassDef(TLFDynGssKT,1)
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ClassDef(TLFDynGssKT,2)
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};
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class TLFDynLorKT : public PUserFcnBase {
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//-----------------------------------------------------------------------------------------------------------------
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/**
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* <p>User function for a dynamic exponential depolarization in a longitudinal field calculated using Laplace transforms
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* See also: Y. J. Uemura, T. Yamazaki, D. R. Harshman, M. Senba, and E. J. Ansaldo,
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* \htmlonly Phys. Rev. B <b>31</b>, 546–563 (1985), doi:<a href="http://dx.doi.org/10.1103/PhysRevB.31.546">10.1103/PhysRevB.31.546</a>
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* \endhtmlonly
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* \latexonly Phys. Rev. B \textbf{31}, 546--563 (1985), \texttt{http://dx.doi.org/10.1103/PhysRevB.31.546}
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* \endlatexonly
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*
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* and: R. S. Hayano, Y. J. Uemura, J. Imazato, N. Nishida, T. Yamazaki, and R. Kubo,
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* \htmlonly Phys. Rev. B <b>20</b>, 850–859 (1979), doi:<a href="http://dx.doi.org/10.1103/PhysRevB.20.850">10.1103/PhysRevB.20.850</a>
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* \endhtmlonly
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* \latexonly Phys. Rev. B \textbf{20}, 850--859 (1979), \texttt{http://dx.doi.org/10.1103/PhysRevB.20.850}
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* \endlatexonly
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*
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* For details regarding the numerical Laplace transform, see e.g.
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* P. Moreno and A. Ramirez,
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* \htmlonly IEEE Trans. Power Delivery <b>23</b>, 2599–2609 (2008), doi:<a href="http://dx.doi.org/10.1109/TPWRD.2008.923404">10.1109/TPWRD.2008.923404</a>
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* \endhtmlonly
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* \latexonly IEEE Trans. Power Delivery \textbf{23}, 2599--2609 (2008), \texttt{http://dx.doi.org/10.1109/TPWRD.2008.923404}
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* \endlatexonly
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*/
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class TLFDynExpKT : public PUserFcnBase {
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public:
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TLFDynLorKT();
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~TLFDynLorKT();
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TLFDynExpKT();
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~TLFDynExpKT();
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Bool_t NeedGlobalPart() const { return false; }
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void SetGlobalPart(vector<void *> &globalPart, UInt_t idx) { }
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@ -129,25 +195,48 @@ public:
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double operator()(double, const vector<double>&) const;
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private:
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mutable vector<double> fPar;
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mutable bool fCalcNeeded;
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mutable bool fFirstCall;
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string fWisdom;
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unsigned int fNSteps;
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double fDt;
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double fDw;
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double fC;
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fftwf_plan fFFTplanFORW;
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fftwf_plan fFFTplanBACK;
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float *fFFTtime;
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fftwf_complex *fFFTfreq;
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mutable unsigned int fCounter;
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mutable double fL1;
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mutable double fL2;
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mutable vector<double> fPar; ///< parameters of the function [\htmlonly ν<sub>L</sub>=<i>B</i>γ<sub>μ</sub>/2π (MHz), <i>a</i> (μs<sup>-1</sup>), ν (MHz)\endhtmlonly \latexonly $\nu_{\mathrm{L}}=B\gamma_{\mu}/2\pi~(\mathrm{MHz})$, $a~(\mu\mathrm{s}^{-1})$, $\nu~(\mathrm{MHz})$ \endlatexonly]
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mutable bool fCalcNeeded; ///< flag indicating if the expensive Laplace transform has to be done (e.g. after parameters have changed)
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mutable bool fFirstCall; ///< flag indicating if the function is evaluated for the first time
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bool fUseWisdom; ///< flag showing if a FFTW3-wisdom file is used
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string fWisdom; ///< path to the wisdom file
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unsigned int fNSteps; ///< length of the Laplace transform
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double fDt; ///< time resolution
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double fDw; ///< frequency resolution
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double fC; ///< coefficient depending on the length of the Laplace transform and time resolution
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fftwf_plan fFFTplanFORW; ///< FFTW3 plan: time domain \htmlonly → \endhtmlonly \latexonly $\rightarrow$ \endlatexonly frequency domain
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fftwf_plan fFFTplanBACK; ///< FFTW3 plan: time domain \htmlonly ← \endhtmlonly \latexonly $\leftarrow$ \endlatexonly frequency domain
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float *fFFTtime; ///< time-domain array
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fftwf_complex *fFFTfreq; ///< frequency-domain array
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mutable unsigned int fCounter; ///< counter determining how many Laplace transforms are done (mainly for debugging purposes)
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mutable double fL1; ///< coefficient used for the high-field and high-hopping-rate approximation
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mutable double fL2; ///< coefficient used for the high-field and high-hopping-rate approximation
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ClassDef(TLFDynLorKT,1)
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ClassDef(TLFDynExpKT,2)
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};
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//-----------------------------------------------------------------------------------------------------------------
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/**
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* <p>User function for a dynamic depolarization in a spin glass in a longitudinal field calculated using Laplace transforms
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* See also: Y. J. Uemura, T. Yamazaki, D. R. Harshman, M. Senba, and E. J. Ansaldo,
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* \htmlonly Phys. Rev. B <b>31</b>, 546–563 (1985), doi:<a href="http://dx.doi.org/10.1103/PhysRevB.31.546">10.1103/PhysRevB.31.546</a>
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* \endhtmlonly
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* \latexonly Phys. Rev. B \textbf{31}, 546--563 (1985), \texttt{http://dx.doi.org/10.1103/PhysRevB.31.546}
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* \endlatexonly
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*
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* and: R. S. Hayano, Y. J. Uemura, J. Imazato, N. Nishida, T. Yamazaki, and R. Kubo,
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* \htmlonly Phys. Rev. B <b>20</b>, 850–859 (1979), doi:<a href="http://dx.doi.org/10.1103/PhysRevB.20.850">10.1103/PhysRevB.20.850</a>
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* \endhtmlonly
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* \latexonly Phys. Rev. B \textbf{20}, 850--859 (1979), \texttt{http://dx.doi.org/10.1103/PhysRevB.20.850}
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* \endlatexonly
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*
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* For details regarding the numerical Laplace transform, see e.g.
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* P. Moreno and A. Ramirez,
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* \htmlonly IEEE Trans. Power Delivery <b>23</b>, 2599–2609 (2008), doi:<a href="http://dx.doi.org/10.1109/TPWRD.2008.923404">10.1109/TPWRD.2008.923404</a>
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* \endhtmlonly
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* \latexonly IEEE Trans. Power Delivery \textbf{23}, 2599--2609 (2008), \texttt{http://dx.doi.org/10.1109/TPWRD.2008.923404}
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* \endlatexonly
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*/
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class TLFDynSG : public PUserFcnBase {
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public:
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@ -161,12 +250,21 @@ public:
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double operator()(double, const vector<double>&) const;
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private:
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mutable vector<double> fPar;
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vector<TLFDynGssKT*> fLFDynGssIntegral;
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mutable vector<double> fPar; ///< parameters of the dynamic Gaussian depolarization function [\htmlonly ν<sub>L</sub>=<i>B</i>γ<sub>μ</sub>/2π (MHz), σ (μs<sup>-1</sup>), ν (MHz)\endhtmlonly \latexonly $\nu_{\mathrm{L}}=B\gamma_{\mu}/2\pi~(\mathrm{MHz})$, $\sigma~(\mu\mathrm{s}^{-1})$, $\nu~(\mathrm{MHz})$ \endlatexonly]
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vector<TLFDynGssKT*> fLFDynGssIntegral; ///< vector of dynamic Gaussian depolarization functions for a subset of static widths
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ClassDef(TLFDynSG,1)
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};
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//-----------------------------------------------------------------------------------------------------------------
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/**
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* <p>User function for a dynamic depolarization in a spin glass in a longitudinal field
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* See also: R. De Renzi and S. Fanesi
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* \htmlonly Physica B <b>289–290</b>, 209–212 (2000), doi:<a href="http://dx.doi.org/10.1016/S0921-4526(00)00368-9">10.1016/S0921-4526(00)00368-9</a>
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* \endhtmlonly
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* \latexonly Physica B \textbf{289--290}, 209--212 (2000), \texttt{http://dx.doi.org/10.1016/S0921-4526(00)00368-9}
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* \endlatexonly
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*/
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class TLFSGInterpolation : public PUserFcnBase {
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public:
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@ -180,10 +278,14 @@ public:
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double operator()(double, const vector<double>&) const;
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private:
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TIntSGInterpolation *fIntegral;
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TIntSGInterpolation *fIntegral; ///< integrator
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mutable map<double, double> fIntValues; ///< previously calculated integral values
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mutable vector<double> fPar; ///< parameters of the function [\htmlonly ν<sub>L</sub>=<i>B</i>γ<sub>μ</sub>/2π (MHz), <i>a</i> (μs<sup>-1</sup>), λ (μs<sup>-1</sup>), β (1) \endhtmlonly \latexonly $\nu_{\mathrm{L}}=B\gamma_{\mu}/2\pi~(\mathrm{MHz})$, $a~(\mu\mathrm{s}^{-1})$, $\lambda~(\mu\mathrm{s}^{-1})$, $\beta~(1)$ \endlatexonly]
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mutable bool fCalcNeeded; ///< flag specifying if an integration has to be done
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mutable double fLastTime; ///< time of the last calculated function value
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ClassDef(TLFSGInterpolation,1)
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ClassDef(TLFSGInterpolation,2)
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};
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#endif //_LFRelaxation_H_
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#endif //_TLFRelaxation_H_
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