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Grid/lib/qcd/action/Actions.h

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Large scale change to support 5d fermion formulations. Have 5d replicated wilson with 4d gauge working and matrix regressing to Ls copies of wilson.
2015-05-31 15:09:02 +01:00
#ifndef GRID_QCD_ACTIONS_H
#define GRID_QCD_ACTIONS_H
Domain wall fermions now invert ; have the basis set up for 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.
2015-06-02 16:57:12 +01:00
// Some reorganisation likely required as both Chroma and IroIro
// are separating the concept of the operator from that of action.
//
// The FermAction contains methods to create
//
// * Linear operators (Hermitian and non-hermitian) .. my LinearOperator
// * System solvers (Hermitian and non-hermitian) .. my OperatorFunction
// * MultiShift System solvers (Hermitian and non-hermitian) .. my OperatorFunction
////////////////////////////////////////////
// Abstract base interface
////////////////////////////////////////////
More progress in the HMC construction
2015-07-03 18:43:14 +01:00
#include <qcd/action/ActionBase.h>
Domain wall fermions now invert ; have the basis set up for 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.
2015-06-02 16:57:12 +01:00
#include <qcd/action/fermion/FermionOperator.h>
More progress in the HMC construction
2015-07-03 18:43:14 +01:00
////////////////////////////////////////////
// Gauge Actions
////////////////////////////////////////////
#include <qcd/action/gauge/WilsonGaugeAction.h>
Domain wall fermions now invert ; have the basis set up for 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.
2015-06-02 16:57:12 +01:00
////////////////////////////////////////////
// Utility functions
////////////////////////////////////////////
#include <qcd/action/fermion/WilsonCompressor.h> //used by all wilson type fermions
#include <qcd/action/fermion/WilsonKernels.h> //used by all wilson type fermions
////////////////////////////////////////////
// 4D formulations
////////////////////////////////////////////
Large scale change to support 5d fermion formulations. Have 5d replicated wilson with 4d gauge working and matrix regressing to Ls copies of wilson.
2015-05-31 15:09:02 +01:00
#include <qcd/action/fermion/WilsonFermion.h>
Domain wall fermions now invert ; have the basis set up for 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.
2015-06-02 16:57:12 +01:00
//#include <qcd/action/fermion/CloverFermion.h>
////////////////////////////////////////////
Overlap Wilson Cayley tanh & zolo
2015-06-03 11:26:54 +01:00
// 5D formulations...
Domain wall fermions now invert ; have the basis set up for 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.
2015-06-02 16:57:12 +01:00
////////////////////////////////////////////
Overlap Wilson Cayley tanh & zolo
2015-06-03 11:26:54 +01:00
Domain wall fermions now invert ; have the basis set up for 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.
2015-06-02 16:57:12 +01:00
#include <qcd/action/fermion/WilsonFermion5D.h> // used by all 5d overlap types
Overlap Wilson Cayley tanh & zolo
2015-06-03 11:26:54 +01:00
//////////
// Cayley
//////////
Domain wall fermions now invert ; have the basis set up for 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.
2015-06-02 16:57:12 +01:00
#include <qcd/action/fermion/CayleyFermion5D.h>
#include <qcd/action/fermion/DomainWallFermion.h>
Mobius Caley form, Mobius Zolotarev operators. Pass Even Odd vs unprec test and hermiticity checks in tests/Grid_any_evenodd.cc; will work on inversion tests shortly.
2015-06-03 09:36:26 +01:00
#include <qcd/action/fermion/DomainWallFermion.h>
Overlap Wilson Cayley tanh & zolo
2015-06-03 11:26:54 +01:00
Mobius Caley form, Mobius Zolotarev operators. Pass Even Odd vs unprec test and hermiticity checks in tests/Grid_any_evenodd.cc; will work on inversion tests shortly.
2015-06-03 09:36:26 +01:00
#include <qcd/action/fermion/MobiusFermion.h>
Scaled Shamir and Scaled Shamir Zolotarev aliases for special cases of Mobius.
2015-06-03 09:51:06 +01:00
#include <qcd/action/fermion/ScaledShamirFermion.h>
Overlap Wilson Cayley tanh & zolo
2015-06-03 11:26:54 +01:00
#include <qcd/action/fermion/OverlapWilsonCayleyTanhFermion.h>
#include <qcd/action/fermion/MobiusZolotarevFermion.h>
#include <qcd/action/fermion/ShamirZolotarevFermion.h>
#include <qcd/action/fermion/OverlapWilsonCayleyZolotarevFermion.h>
//////////////////////
// Continued fraction
//////////////////////
#include <qcd/action/fermion/ContinuedFractionFermion5D.h>
Implementing the Hw kernel continued fraction 5d overlap cases
2015-06-04 00:23:16 +01:00
#include <qcd/action/fermion/OverlapWilsonContfracTanhFermion.h>
#include <qcd/action/fermion/OverlapWilsonContfracZolotarevFermion.h>
Overlap Wilson Cayley tanh & zolo
2015-06-03 11:26:54 +01:00
//////////////////////
// Partial fraction
//////////////////////
#include <qcd/action/fermion/PartialFractionFermion5D.h>
PartialFraction Hw with Zolo and Tanh approx converged under CG and passed EO breakdown and hermiticity tests.
2015-06-04 13:28:37 +01:00
#include <qcd/action/fermion/OverlapWilsonPartialFractionTanhFermion.h>
#include <qcd/action/fermion/OverlapWilsonPartialFractionZolotarevFermion.h>
Domain wall fermions now invert ; have the basis set up for 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.
2015-06-02 16:57:12 +01:00
Conjugate residual added
2015-06-05 18:16:25 +01:00
///////////////////////////////////////////////////////////////////////////////
// G5 herm -- this has to live in QCD since dirac matrix is not in the broader sector of code
///////////////////////////////////////////////////////////////////////////////
#include <qcd/action/fermion/g5HermitianLinop.h>
Domain wall fermions now invert ; have the basis set up for 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.
2015-06-02 16:57:12 +01:00
Two flavour HMC for Wilson/Wilson is conserving energy. Still to check plaq and <e(-dH)>, but nevertheless this is progress
2015-07-29 09:53:39 +01:00
////////////////////////////////////////
// Pseudo fermion combinations
////////////////////////////////////////
#include <qcd/action/pseudofermion/TwoFlavour.h>
Adding components for even odd decomposed determinant in HMC. dH not yet conserved, so something wrong in the eo force code still
2015-08-07 08:37:15 +01:00
#include <qcd/action/pseudofermion/TwoFlavourEvenOdd.h>
Two flavour HMC for Wilson/Wilson is conserving energy. Still to check plaq and <e(-dH)>, but nevertheless this is progress
2015-07-29 09:53:39 +01:00
Large scale change to support 5d fermion formulations. Have 5d replicated wilson with 4d gauge working and matrix regressing to Ls copies of wilson.
2015-05-31 15:09:02 +01:00
#endif
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