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Grid/lib/qcd/action/pseudofermion/TwoFlavourRatio.h

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/*************************************************************************************
Grid physics library, www.github.com/paboyle/Grid
Source file: ./lib/qcd/action/pseudofermion/TwoFlavourRatio.h
Copyright (C) 2015
Author: Peter Boyle <paboyle@ph.ed.ac.uk>
Author: Peter Boyle <peterboyle@Peters-MacBook-Pro-2.local>
Author: paboyle <paboyle@ph.ed.ac.uk>
This program 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 2 of the License, or
(at your option) any later version.
This program 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, write to the Free Software Foundation, Inc.,
51 Franklin Street, Fifth Floor, Boston, MA 02110-1301 USA.
See the full license in the file "LICENSE" in the top level distribution directory
*************************************************************************************/
/* END LEGAL */
#ifndef QCD_PSEUDOFERMION_TWO_FLAVOUR_RATIO_H
#define QCD_PSEUDOFERMION_TWO_FLAVOUR_RATIO_H
namespace Grid{
namespace QCD{
///////////////////////////////////////
// Two flavour ratio
///////////////////////////////////////
template<class Impl>
class TwoFlavourRatioPseudoFermionAction : public Action<typename Impl::GaugeField> {
public:
INHERIT_IMPL_TYPES(Impl);
private:
FermionOperator<Impl> & NumOp;// the basic operator
FermionOperator<Impl> & DenOp;// the basic operator
OperatorFunction<FermionField> &DerivativeSolver;
OperatorFunction<FermionField> &ActionSolver;
FermionField Phi; // the pseudo fermion field for this trajectory
public:
TwoFlavourRatioPseudoFermionAction(FermionOperator<Impl> &_NumOp,
FermionOperator<Impl> &_DenOp,
OperatorFunction<FermionField> & DS,
OperatorFunction<FermionField> & AS
) : NumOp(_NumOp), DenOp(_DenOp), DerivativeSolver(DS), ActionSolver(AS), Phi(_NumOp.FermionGrid()) {};
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virtual std::string action_name(){return "TwoFlavourRatioPseudoFermionAction";}
virtual std::string LogParameters(){
std::stringstream sstream;
sstream << GridLogMessage << "["<<action_name()<<"] has no parameters" << std::endl;
return sstream.str();
}
virtual void refresh(const GaugeField &U, GridParallelRNG& pRNG) {
// P(phi) = e^{- phi^dag V (MdagM)^-1 Vdag phi}
//
// NumOp == V
// DenOp == M
//
// Take phi = Vdag^{-1} Mdag eta ; eta = Mdag^{-1} Vdag Phi
//
// P(eta) = e^{- eta^dag eta}
//
// e^{x^2/2 sig^2} => sig^2 = 0.5.
//
// So eta should be of width sig = 1/sqrt(2) and must multiply by 0.707....
//
RealD scale = std::sqrt(0.5);
FermionField eta(NumOp.FermionGrid());
FermionField tmp(NumOp.FermionGrid());
gaussian(pRNG,eta);
NumOp.ImportGauge(U);
DenOp.ImportGauge(U);
// Note: this hard codes normal equations type solvers; alternate implementation needed for
// non-herm style solvers.
MdagMLinearOperator<FermionOperator<Impl> ,FermionField> MdagMOp(NumOp);
DenOp.Mdag(eta,Phi); // Mdag eta
tmp = zero;
ActionSolver(MdagMOp,Phi,tmp); // (VdagV)^-1 Mdag eta = V^-1 Vdag^-1 Mdag eta
NumOp.M(tmp,Phi); // Vdag^-1 Mdag eta
Phi=Phi*scale;
};
//////////////////////////////////////////////////////
// S = phi^dag V (Mdag M)^-1 Vdag phi
//////////////////////////////////////////////////////
virtual RealD S(const GaugeField &U) {
NumOp.ImportGauge(U);
DenOp.ImportGauge(U);
FermionField X(NumOp.FermionGrid());
FermionField Y(NumOp.FermionGrid());
MdagMLinearOperator<FermionOperator<Impl> ,FermionField> MdagMOp(DenOp);
NumOp.Mdag(Phi,Y); // Y= Vdag phi
X=zero;
ActionSolver(MdagMOp,Y,X); // X= (MdagM)^-1 Vdag phi
DenOp.M(X,Y); // Y= Mdag^-1 Vdag phi
RealD action = norm2(Y);
return action;
};
//////////////////////////////////////////////////////
// dS/du = phi^dag dV (Mdag M)^-1 V^dag phi
// - phi^dag V (Mdag M)^-1 [ Mdag dM + dMdag M ] (Mdag M)^-1 V^dag phi
// + phi^dag V (Mdag M)^-1 dV^dag phi
//////////////////////////////////////////////////////
virtual void deriv(const GaugeField &U,GaugeField & dSdU) {
NumOp.ImportGauge(U);
DenOp.ImportGauge(U);
MdagMLinearOperator<FermionOperator<Impl> ,FermionField> MdagMOp(DenOp);
FermionField X(NumOp.FermionGrid());
FermionField Y(NumOp.FermionGrid());
GaugeField force(NumOp.GaugeGrid());
//Y=Vdag phi
//X = (Mdag M)^-1 V^dag phi
//Y = (Mdag)^-1 V^dag phi
NumOp.Mdag(Phi,Y); // Y= Vdag phi
X=zero;
DerivativeSolver(MdagMOp,Y,X); // X= (MdagM)^-1 Vdag phi
DenOp.M(X,Y); // Y= Mdag^-1 Vdag phi
// phi^dag V (Mdag M)^-1 dV^dag phi
NumOp.MDeriv(force , X, Phi, DaggerYes ); dSdU=force;
// phi^dag dV (Mdag M)^-1 V^dag phi
NumOp.MDeriv(force , Phi, X ,DaggerNo ); dSdU=dSdU+force;
// - phi^dag V (Mdag M)^-1 Mdag dM (Mdag M)^-1 V^dag phi
// - phi^dag V (Mdag M)^-1 dMdag M (Mdag M)^-1 V^dag phi
DenOp.MDeriv(force,Y,X,DaggerNo); dSdU=dSdU-force;
DenOp.MDeriv(force,X,Y,DaggerYes); dSdU=dSdU-force;
dSdU *= -1.0;
//dSdU = - Ta(dSdU);
};
};
}
}
#endif