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2583570e17
Tanh/Zolo * (Cayley/PartFrac/ContFrac) * (Mobius/Shamir/Wilson) Approx Representation Kernel. All are done with space-time taking part in checkerboarding, Ls uncheckerboarded Have only so far tested the Domain Wall limit of mobius, and at that only checked that it i) Inverts ii) 5dim DW == Ls copies of 4dim D2 iii) MeeInv Mee == 1 iv) Meo+Mee+Moe+Moo == M unprec. v) MpcDagMpc is hermitan vi) Mdag is the adjoint of M between stochastic vectors. That said, the RB schur solve, RB MpcDagMpc solve, Unprec solve all converge and the true residual becomes small; so pretty good tests.
120 lines
3.6 KiB
C++
120 lines
3.6 KiB
C++
#include <Grid.h>
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namespace Grid {
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namespace QCD {
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RealD ContinuedFractionFermion5D::M (const LatticeFermion &psi, LatticeFermion &chi)
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{
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LatticeFermion D(psi._grid);
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DW(psi,D,DaggerNo);
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int sign=1;
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for(int s=0;s<Ls;s++){
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if ( s==0 ) {
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ag5xpby_ssp(chi,cc[0]*Beta[0]*sign*scale,D,sqrt_cc[0],psi,s,s+1); // Multiplies Dw by G5 so Hw
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} else if ( s==(Ls-1) ){
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RealD R=(1.0+mass)/(1.0-mass);
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ag5xpby_ssp(chi,Beta[s]*scale,D,sqrt_cc[s-1],psi,s,s-1);
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ag5xpby_ssp(chi,R,psi,1.0,chi,s,s);
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} else {
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ag5xpby_ssp(chi,cc[s]*Beta[s]*sign*scale,D,sqrt_cc[s],psi,s,s+1);
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axpby_ssp(chi,1.0,chi,sqrt_cc[s-1],psi,s,s-1);
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}
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sign=-sign;
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}
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return norm2(chi);
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}
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RealD ContinuedFractionFermion5D::Mdag (const LatticeFermion &psi, LatticeFermion &chi)
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{
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// This matrix is already hermitian. (g5 Dw) = Dw dag g5 = (g5 Dw)dag
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// The rest of matrix is symmetric.
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// Can ignore "dag"
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return M(psi,chi);
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}
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void ContinuedFractionFermion5D::Meooe (const LatticeFermion &psi, LatticeFermion &chi)
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{
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Dhop(psi,chi,DaggerNo); // Dslash on diagonal. g5 Dslash is hermitian
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int sign=1;
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for(int s=0;s<Ls;s++){
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if ( s==(Ls-1) ){
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ag5xpby_ssp(chi,Beta[s]*scale,chi,0.0,chi,s,s);
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} else {
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ag5xpby_ssp(chi,cc[s]*Beta[s]*sign*scale,chi,0.0,chi,s,s);
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}
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sign=-sign;
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}
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}
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void ContinuedFractionFermion5D::MeooeDag (const LatticeFermion &psi, LatticeFermion &chi)
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{
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Meooe(psi,chi);
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}
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void ContinuedFractionFermion5D::Mooee (const LatticeFermion &psi, LatticeFermion &chi)
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{
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double dw_diag = (4.0-this->M5)*scale;
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int sign=1;
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for(int s=0;s<Ls;s++){
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if ( s==0 ) {
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ag5xpby_ssp(chi,cc[0]*Beta[0]*sign*dw_diag,psi,sqrt_cc[0],psi,s,s+1); // Multiplies Dw by G5 so Hw
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} else if ( s==(Ls-1) ){
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// Drop the CC here.
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double R=(1+this->mass)/(1-this->mass);
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ag5xpby_ssp(chi,Beta[s]*dw_diag,psi,sqrt_cc[s-1],psi,s,s-1);
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ag5xpby_ssp(chi,R,psi,1.0,chi,s,s);
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} else {
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ag5xpby_ssp(chi,cc[s]*Beta[s]*sign*dw_diag,psi,sqrt_cc[s],psi,s,s+1);
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axpby_ssp(chi,1.0,chi,sqrt_cc[s-1],psi,s,s-1);
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}
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sign=-sign;
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}
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}
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void ContinuedFractionFermion5D::MooeeDag (const LatticeFermion &psi, LatticeFermion &chi)
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{
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Mooee(psi,chi);
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}
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void ContinuedFractionFermion5D::MooeeInv (const LatticeFermion &psi, LatticeFermion &chi)
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{
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// Apply Linv
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axpby_ssp(chi,1.0/cc_d[0],psi,0.0,psi,0,0);
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for(int s=1;s<Ls;s++){
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axpbg5y_ssp(chi,1.0/cc_d[s],psi,-1.0/See[s-1],chi,s,s-1);
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}
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// Apply Dinv
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for(int s=0;s<Ls;s++){
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ag5xpby_ssp(chi,1.0/See[s],chi,0.0,chi,s,s); //only appearance of See[0]
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}
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// Apply Uinv = (Linv)^T
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axpby_ssp(chi,1.0/cc_d[Ls-1],chi,0.0,chi,this->Ls-1,this->Ls-1);
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for(int s=Ls-2;s>=0;s--){
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axpbg5y_ssp(chi,1.0/cc_d[s],chi,-1.0*cc_d[s+1]/See[s]/cc_d[s],chi,s,s+1);
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}
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}
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void ContinuedFractionFermion5D::MooeeInvDag (const LatticeFermion &psi, LatticeFermion &chi)
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{
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MooeeInv(psi,chi);
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}
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// Constructors
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ContinuedFractionFermion5D::ContinuedFractionFermion5D(
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LatticeGaugeField &_Umu,
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GridCartesian &FiveDimGrid,
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GridRedBlackCartesian &FiveDimRedBlackGrid,
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GridCartesian &FourDimGrid,
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GridRedBlackCartesian &FourDimRedBlackGrid,
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RealD _mass,RealD M5) :
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WilsonFermion5D(_Umu,
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FiveDimGrid, FiveDimRedBlackGrid,
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FourDimGrid, FourDimRedBlackGrid,M5),
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mass(_mass)
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{
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}
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}
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}
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