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Provides the DDHMC lexicon for a pair of non-Dirichlet and Dirichlet operators

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Peter Boyle 2021-05-11 13:54:49 -04:00
parent 94a2a645bd
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/*************************************************************************************
Grid physics library, www.github.com/paboyle/Grid
Source file: ./lib/qcd/action/fermion/SchurFactoredFermionOperator.h
Copyright (C) 2021
Author: Peter Boyle <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 */
#pragma once
NAMESPACE_BEGIN(Grid);
////////////////////////////////////////////////////////
// Some explanation of class structure for domain decomposition:
//
// Need a dirichlet operator for two flavour determinant - acts on both Omega and OmegaBar.
//
// Possible gain if the global sums and CG are run independently?? Could measure this.
//
// Types of operations
//
// 1) assemble local det dOmega det dOmegaBar pseudofermion
//
// - DirichletFermionOperator - can either do a global solve, or independent/per cell coefficients.
//
// 2) assemble dOmegaInverse and dOmegaBarInverse in R
//
// - DirichletFermionOperator - can also be used to
// - need two or more cells per node. Options
// - a) solve one cell at a time, no new code, CopyRegion and reduced /split Grids
// - b) solve multiple cells in parallel. predicated dslash implementation
//
// - b) has more parallelism, experience with block solver suggest might not be aalgorithmically inefficient
// a) has more cache friendly and easier code.
// b) is easy to implement in a "trial" or inefficient code with projection.
//
// 3) Additional functionality for domain operations
//
// - SchurFactoredFermionOperator - Need a DDHMC utility - whether used in two flavour or one flavour
//
// - dBoundary - needs non-dirichlet operator
// - Contains one Dirichlet Op, and one non-Dirichlet op. Implements dBoundary etc...
// - The Dirichlet ops can be passed to dOmega(Bar) solvers etc...
//
////////////////////////////////////////////////////////
template<class Impl>
class SchurFactoredFermionOperator : public Impl
{
INHERIT_IMPL_TYPES(Impl);
FermionOperator<Impl> & DirichletFermOp;
FermionOperator<Impl> & FermOp;
OperatorFunction<FermionField> &Solver;
Coordinate Block;
public:
SchurFactoredFermionOperator(FermionOperator<Impl> & _FermOp,
FermionOperator<Impl> & _DirichletFermOp,
OperatorFunction<FermionField> &_Solver,
Coordinate & _Block)
: Block(_Block),
FermOp(_FermOp),
DirichletFermOp(_DirichletFermOp),
Solver(_Solver)
{
// FIXME -- could check that the DirichletFermOp block matches this.
// Pass in Dirichlet FermOp because we really need two dirac operators
// as double stored gauge fields differ.
};
enum Domain { Omega=0, OmegaBar=1 };
void ImportGauge(const GaugeField &Umu)
{
FermOp.ImportGauge(Umu);
DirichletFermOp.ImportGauge(Umu);
}
void ProjectBoundaryBothDomains (FermionField &f,int sgn)
{
assert((sgn==1)||(sgn==-1));
Real rsgn = sgn;
Gamma::Algebra Gmu [] = {
Gamma::Algebra::GammaX,
Gamma::Algebra::GammaY,
Gamma::Algebra::GammaZ,
Gamma::Algebra::GammaT
};
GridBase *grid = f.Grid();
LatticeInteger coor(grid);
LatticeInteger face(grid);
LatticeInteger one(grid); one = 1;
LatticeInteger zero(grid); zero = 0;
LatticeInteger nface(grid); nface=Zero();
ComplexField zz(grid); zz=Zero();
FermionField projected(grid); projected=Zero();
FermionField sp_proj (grid);
int dims = grid->Nd();
int isDWF= (dims==Nd+1);
assert((dims==Nd)||(dims==Nd+1));
for(int mu=0;mu<Nd;mu++){
// need to worry about DWF 5th dim first
LatticeCoordinate(coor,mu+isDWF);
face = where(mod(coor,Block[mu]) == Integer(0),one,zero );
nface = nface + face;
Gamma G(Gmu[mu]);
// Lower face receives (1-gamma)/2 in normal forward hopping term
sp_proj = 0.5*(f-G*f*rsgn);
projected= where(face,sp_proj,projected);
face = where(mod(coor,Block[mu]) == Integer(Block[mu]-1) ,one,zero );
nface = nface + face;
// Upper face receives (1+gamma)/2 in normal backward hopping term
sp_proj = 0.5*(f+G*f*rsgn);
projected= where(face,sp_proj,projected);
}
// Initial Zero() where nface==0.
// Keep the spin projected faces where nface==1
// Full spinor where nface>=2
projected = where(nface>Integer(1),f,projected);
}
void ProjectDomain(FermionField &f,int domain)
{
GridBase *grid = f.Grid();
int dims = grid->Nd();
int isDWF= (dims==Nd+1);
assert((dims==Nd)||(dims==Nd+1));
FermionField zz(grid); zz=Zero();
LatticeInteger coor(grid);
LatticeInteger domaincb(grid); domaincb=Zero();
for(int d=0;d<Nd;d++){
LatticeCoordinate(coor,d+isDWF);
domaincb = domaincb + div(coor,Block[d]);
}
f = where(mod(domaincb,2)==Integer(domain),f,zz);
};
void ProjectOmegaBar (FermionField &f) {ProjectDomain(f,OmegaBar);}
void ProjectOmega (FermionField &f) {ProjectDomain(f,Omega);}
// See my notes(!).
// Notation: Following Luscher, we introduce projectors $\hPdb$ with both spinor and space structure
// projecting all spinor elements in $\Omega$ connected by $\Ddb$ to $\bar{\Omega}$,
void ProjectBoundaryBar(FermionField &f)
{
ProjectBoundaryBothDomains(f,1);
ProjectOmega(f);
}
// and $\hPd$ projecting all spinor elements in $\bar{\Omega}$ connected by $\Dd$ to $\Omega$.
void ProjectBoundary (FermionField &f)
{
ProjectBoundaryBothDomains(f,1);
ProjectOmegaBar(f);
};
void dBoundary (FermionField &in,FermionField &out)
{
FermionField tmp(in);
ProjectOmegaBar(tmp);
FermOp.M(tmp,out);
ProjectOmega(out);
};
void dBoundaryDag (FermionField &in,FermionField &out)
{
FermionField tmp(in);
ProjectOmega(tmp);
FermOp.Mdag(tmp,out);
ProjectOmegaBar(out);
};
void dBoundaryBar (FermionField &in,FermionField &out)
{
FermionField tmp(in);
ProjectOmega(tmp);
FermOp.M(tmp,out);
ProjectOmegaBar(out);
};
void dBoundaryBarDag (FermionField &in,FermionField &out)
{
FermionField tmp(in);
ProjectOmegaBar(tmp);
FermOp.Mdag(tmp,out);
ProjectOmega(out);
};
void dOmega (FermionField &in,FermionField &out)
{
FermionField tmp(in);
ProjectOmega(tmp);
DirichletFermOp.M(tmp,out);
ProjectOmega(out);
};
void dOmegaBar (FermionField &in,FermionField &out)
{
FermionField tmp(in);
ProjectOmegaBar(tmp);
DirichletFermOp.M(tmp,out);
ProjectOmegaBar(out);
};
void dOmegaDag (FermionField &in,FermionField &out)
{
FermionField tmp(in);
ProjectOmega(tmp);
DirichletFermOp.Mdag(tmp,out);
ProjectOmega(out);
};
void dOmegaBarDag (FermionField &in,FermionField &out)
{
FermionField tmp(in);
ProjectOmegaBar(tmp);
DirichletFermOp.Mdag(tmp,out);
ProjectOmegaBar(out);
};
void dOmegaInv (FermionField &in,FermionField &out)
{
FermionField tmp(in);
ProjectOmega(tmp);
dOmegaInvAndOmegaBarInv(tmp,out); // Inefficient warning
ProjectOmega(out);
};
void dOmegaBarInv(FermionField &in,FermionField &out)
{
FermionField tmp(in);
ProjectOmegaBar(tmp);
dOmegaInvAndOmegaBarInv(tmp,out);
ProjectOmegaBar(out);
};
void dOmegaDagInv (FermionField &in,FermionField &out)
{
FermionField tmp(in);
ProjectOmega(tmp);
dOmegaDagInvAndOmegaBarDagInv(tmp,out);
ProjectOmega(out);
};
void dOmegaBarDagInv(FermionField &in,FermionField &out)
{
FermionField tmp(in);
ProjectOmegaBar(tmp);
dOmegaDagInvAndOmegaBarDagInv(tmp,out);
ProjectOmegaBar(out);
};
void dOmegaInvAndOmegaBarInv(FermionField &in,FermionField &out)
{
SchurRedBlackDiagMooeeSolve<FermionField> PrecSolve(Solver);
PrecSolve(DirichletFermOp,in,out);
};
void dOmegaDagInvAndOmegaBarDagInv(FermionField &in,FermionField &out)
{
SchurRedBlackDiagMooeeDagSolve<FermionField> PrecSolve(Solver);
PrecSolve(DirichletFermOp,in,out);
};
// Rdag = Pdbar - DdbarDag DomegabarDagInv DdDag DomegaDagInv Pdbar
void RDag(FermionField &in,FermionField &out)
{
FermionField tmp1(FermOp.FermionGrid());
FermionField tmp2(FermOp.FermionGrid());
out = in; ProjectBoundaryBar(out);
dOmegaDagInv(out,tmp1);
dBoundaryDag(tmp1,tmp2);
dOmegaBarDagInv(tmp2,tmp1);
dBoundaryBarDag(tmp1,tmp2);
out = out - tmp2;
};
// R = Pdbar - Pdbar DomegaInv Dd DomegabarInv Ddbar
void R(FermionField &in,FermionField &out)
{
FermionField tmp1(FermOp.FermionGrid());
FermionField tmp2(FermOp.FermionGrid());
out = in;
ProjectBoundaryBar(out);
dBoundaryBar(out,tmp1);
dOmegaBarInv(tmp1,tmp2);
dBoundary(tmp2,tmp1);
dOmegaInv(tmp1,tmp2);
out = in - tmp2 ;
ProjectBoundaryBar(out);
};
// R = Pdbar - Pdbar Dinv Ddbar
void RInv(FermionField &in,FermionField &out)
{
FermionField tmp1(FermOp.FermionGrid());
dBoundaryBar(in,out);
Dinverse(out,tmp1);
out =in -tmp1;
ProjectBoundaryBar(out);
};
// R = Pdbar - DdbarDag DinvDag Pdbar
void RDagInv(FermionField &in,FermionField &out)
{
FermionField tmp(FermOp.FermionGrid());
FermionField Pin(FermOp.FermionGrid());
Pin = in; ProjectBoundaryBar(Pin);
DinverseDag(Pin,out);
dBoundaryBarDag(out,tmp);
out =Pin -tmp;
};
void Dinverse(FermionField &in,FermionField &out)
{
SchurRedBlackDiagMooeeSolve<FermionField> Solve(Solver);
Solve(FermOp,in,out);
}
void DinverseDag(FermionField &in,FermionField &out)
{
SchurRedBlackDiagMooeeDagSolve<FermionField> Solve(Solver);
Solve(FermOp,in,out);
}
};
NAMESPACE_END(Grid);