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Grid/lib/qcd/action/fermion/Fermion.h

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Global edit adding copyright and license info to every source file.
2016-01-02 14:51:32 +00:00
/*************************************************************************************
Grid physics library, www.github.com/paboyle/Grid
Refactoring header layout
2017-02-22 18:09:33 +00:00
Source file: ./lib/qcd/action/fermion/Fermion_base_aggregate.h
Global edit adding copyright and license info to every source file.
2016-01-02 14:51:32 +00:00
Copyright (C) 2015
Author: Peter Boyle <pabobyle@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 */
Merge branch 'develop' into feature/bgq-asm
2017-02-23 00:25:29 +00:00
#ifndef GRID_QCD_FERMION_H
#define GRID_QCD_FERMION_H
Global edit on HMC sector -- making GaugeField a template parameter and preparing to pass integrator, smearing, bc's as policy classes to hmc. Propose to unify "integrator" and integrator algorithm in a base/derived way to override step. Want to read through ForceGradient to ensure that abstraction covers the force gradient case.
2015-08-30 12:18:34 +01:00
Rework/global edit to enforce type templating of fermion operators. Allows multi-precision work and paves the way for alternate BC's and such like allowing for example G-parity which is important for K pipi programme. In particular, can drive an extra flavour index into the fermion fields using template types.
2015-08-10 20:47:44 +01:00
////////////////////////////////////////////////////////////////////////////////////////////////////
// Explicit explicit template instantiation is still required in the .cc files
//
// - CayleyFermion5D.cc
// - PartialFractionFermion5D.cc
// - WilsonFermion5D.cc
// - WilsonKernelsHand.cc
// - ContinuedFractionFermion5D.cc
// - WilsonFermion.cc
// - WilsonKernels.cc
//
// The explicit instantiation is only avoidable if we move this source to headers and end up with include/parse/recompile
// for EVERY .cc file. This define centralises the list and restores global push of impl cases
////////////////////////////////////////////////////////////////////////////////////////////////////
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
////////////////////////////////////////////
Rework/global edit to enforce type templating of fermion operators. Allows multi-precision work and paves the way for alternate BC's and such like allowing for example G-parity which is important for K pipi programme. In particular, can drive an extra flavour index into the fermion fields using template types.
2015-08-10 20:47:44 +01:00
// Fermion operators / actions
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
Open up dependency on Eigen and FFTW
2016-07-07 22:31:07 +01:00
#include <Grid/qcd/action/fermion/WilsonFermion.h> // 4d wilson like
#include <Grid/qcd/action/fermion/WilsonTMFermion.h> // 4d wilson like
#include <Grid/qcd/action/fermion/WilsonFermion5D.h> // 5d base used by all 5d overlap types
//#include <Grid/qcd/action/fermion/CloverFermion.h>
Staggered
2016-11-01 14:24:22 +00:00
#include <Grid/qcd/action/fermion/ImprovedStaggeredFermion.h>
Staggerd Fermion 5D
2016-11-29 13:13:56 +00:00
#include <Grid/qcd/action/fermion/ImprovedStaggeredFermion5D.h>
Open up dependency on Eigen and FFTW
2016-07-07 22:31:07 +01:00
#include <Grid/qcd/action/fermion/CayleyFermion5D.h> // Cayley types
#include <Grid/qcd/action/fermion/DomainWallFermion.h>
#include <Grid/qcd/action/fermion/DomainWallFermion.h>
#include <Grid/qcd/action/fermion/MobiusFermion.h>
Feature for z-Mobius prep
2016-08-15 22:31:29 +01:00
#include <Grid/qcd/action/fermion/ZMobiusFermion.h>
Open up dependency on Eigen and FFTW
2016-07-07 22:31:07 +01:00
#include <Grid/qcd/action/fermion/ScaledShamirFermion.h>
#include <Grid/qcd/action/fermion/MobiusZolotarevFermion.h>
#include <Grid/qcd/action/fermion/ShamirZolotarevFermion.h>
#include <Grid/qcd/action/fermion/OverlapWilsonCayleyTanhFermion.h>
#include <Grid/qcd/action/fermion/OverlapWilsonCayleyZolotarevFermion.h>
#include <Grid/qcd/action/fermion/ContinuedFractionFermion5D.h> // Continued fraction
#include <Grid/qcd/action/fermion/OverlapWilsonContfracTanhFermion.h>
#include <Grid/qcd/action/fermion/OverlapWilsonContfracZolotarevFermion.h>
#include <Grid/qcd/action/fermion/PartialFractionFermion5D.h> // Partial fraction
#include <Grid/qcd/action/fermion/OverlapWilsonPartialFractionTanhFermion.h>
#include <Grid/qcd/action/fermion/OverlapWilsonPartialFractionZolotarevFermion.h>
Refactoring header layout
2017-02-22 18:09:33 +00:00
///////////////////////////////////////////////////////////////////////////////
// G5 herm -- this has to live in QCD since dirac matrix is not in the broader sector of code
///////////////////////////////////////////////////////////////////////////////
#include <Grid/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
Rework/global edit to enforce type templating of fermion operators. Allows multi-precision work and paves the way for alternate BC's and such like allowing for example G-parity which is important for K pipi programme. In particular, can drive an extra flavour index into the fermion fields using template types.
2015-08-10 20:47:44 +01:00
////////////////////////////////////////////////////////////////////////////////////////////////////
// More maintainable to maintain the following typedef list centrally, as more "impl" targets
// are added, (e.g. extension for gparity, half precision project in comms etc..)
////////////////////////////////////////////////////////////////////////////////////////////////////
// Cayley 5d
namespace Grid {
namespace QCD {
typedef WilsonFermion<WilsonImplR> WilsonFermionR;
typedef WilsonFermion<WilsonImplF> WilsonFermionF;
typedef WilsonFermion<WilsonImplD> WilsonFermionD;
Modified the Dirac Kernel class to compile with different number of colours Added the general push_back functionality to accomodate for all defined representations Compiles, not tested
2016-07-18 16:36:28 +01:00
typedef WilsonFermion<WilsonAdjImplR> WilsonAdjFermionR;
typedef WilsonFermion<WilsonAdjImplF> WilsonAdjFermionF;
typedef WilsonFermion<WilsonAdjImplD> WilsonAdjFermionD;
Added support for the Two index Symmetric and Antisymmetric representations Tested for HMC convergence: OK Added also a test file showing an example for mixed representations
2016-09-22 14:17:37 +01:00
typedef WilsonFermion<WilsonTwoIndexSymmetricImplR> WilsonTwoIndexSymmetricFermionR;
typedef WilsonFermion<WilsonTwoIndexSymmetricImplF> WilsonTwoIndexSymmetricFermionF;
typedef WilsonFermion<WilsonTwoIndexSymmetricImplD> WilsonTwoIndexSymmetricFermionD;
Wilson TM tests and compiles in
2015-12-17 23:06:33 +00:00
typedef WilsonTMFermion<WilsonImplR> WilsonTMFermionR;
typedef WilsonTMFermion<WilsonImplF> WilsonTMFermionF;
typedef WilsonTMFermion<WilsonImplD> WilsonTMFermionD;
Rework/global edit to enforce type templating of fermion operators. Allows multi-precision work and paves the way for alternate BC's and such like allowing for example G-parity which is important for K pipi programme. In particular, can drive an extra flavour index into the fermion fields using template types.
2015-08-10 20:47:44 +01:00
typedef DomainWallFermion<WilsonImplR> DomainWallFermionR;
typedef DomainWallFermion<WilsonImplF> DomainWallFermionF;
typedef DomainWallFermion<WilsonImplD> DomainWallFermionD;
Actions updated
2016-11-29 00:14:36 +00:00
Rework/global edit to enforce type templating of fermion operators. Allows multi-precision work and paves the way for alternate BC's and such like allowing for example G-parity which is important for K pipi programme. In particular, can drive an extra flavour index into the fermion fields using template types.
2015-08-10 20:47:44 +01:00
typedef MobiusFermion<WilsonImplR> MobiusFermionR;
typedef MobiusFermion<WilsonImplF> MobiusFermionF;
typedef MobiusFermion<WilsonImplD> MobiusFermionD;
Feature for z-Mobius prep
2016-08-15 22:31:29 +01:00
typedef ZMobiusFermion<ZWilsonImplR> ZMobiusFermionR;
typedef ZMobiusFermion<ZWilsonImplF> ZMobiusFermionF;
typedef ZMobiusFermion<ZWilsonImplD> ZMobiusFermionD;
Actions updated
2016-11-29 00:14:36 +00:00
// Ls vectorised
typedef DomainWallFermion<DomainWallVec5dImplR> DomainWallFermionVec5dR;
typedef DomainWallFermion<DomainWallVec5dImplF> DomainWallFermionVec5dF;
typedef DomainWallFermion<DomainWallVec5dImplD> DomainWallFermionVec5dD;
typedef MobiusFermion<DomainWallVec5dImplR> MobiusFermionVec5dR;
typedef MobiusFermion<DomainWallVec5dImplF> MobiusFermionVec5dF;
typedef MobiusFermion<DomainWallVec5dImplD> MobiusFermionVec5dD;
typedef ZMobiusFermion<ZDomainWallVec5dImplR> ZMobiusFermionVec5dR;
typedef ZMobiusFermion<ZDomainWallVec5dImplF> ZMobiusFermionVec5dF;
typedef ZMobiusFermion<ZDomainWallVec5dImplD> ZMobiusFermionVec5dD;
Rework/global edit to enforce type templating of fermion operators. Allows multi-precision work and paves the way for alternate BC's and such like allowing for example G-parity which is important for K pipi programme. In particular, can drive an extra flavour index into the fermion fields using template types.
2015-08-10 20:47:44 +01:00
typedef ScaledShamirFermion<WilsonImplR> ScaledShamirFermionR;
typedef ScaledShamirFermion<WilsonImplF> ScaledShamirFermionF;
typedef ScaledShamirFermion<WilsonImplD> ScaledShamirFermionD;
typedef MobiusZolotarevFermion<WilsonImplR> MobiusZolotarevFermionR;
typedef MobiusZolotarevFermion<WilsonImplF> MobiusZolotarevFermionF;
typedef MobiusZolotarevFermion<WilsonImplD> MobiusZolotarevFermionD;
typedef ShamirZolotarevFermion<WilsonImplR> ShamirZolotarevFermionR;
typedef ShamirZolotarevFermion<WilsonImplF> ShamirZolotarevFermionF;
typedef ShamirZolotarevFermion<WilsonImplD> ShamirZolotarevFermionD;
typedef OverlapWilsonCayleyTanhFermion<WilsonImplR> OverlapWilsonCayleyTanhFermionR;
typedef OverlapWilsonCayleyTanhFermion<WilsonImplF> OverlapWilsonCayleyTanhFermionF;
typedef OverlapWilsonCayleyTanhFermion<WilsonImplD> OverlapWilsonCayleyTanhFermionD;
typedef OverlapWilsonCayleyZolotarevFermion<WilsonImplR> OverlapWilsonCayleyZolotarevFermionR;
typedef OverlapWilsonCayleyZolotarevFermion<WilsonImplF> OverlapWilsonCayleyZolotarevFermionF;
typedef OverlapWilsonCayleyZolotarevFermion<WilsonImplD> OverlapWilsonCayleyZolotarevFermionD;
// Continued fraction
typedef OverlapWilsonContFracTanhFermion<WilsonImplR> OverlapWilsonContFracTanhFermionR;
typedef OverlapWilsonContFracTanhFermion<WilsonImplF> OverlapWilsonContFracTanhFermionF;
typedef OverlapWilsonContFracTanhFermion<WilsonImplD> OverlapWilsonContFracTanhFermionD;
typedef OverlapWilsonContFracZolotarevFermion<WilsonImplR> OverlapWilsonContFracZolotarevFermionR;
typedef OverlapWilsonContFracZolotarevFermion<WilsonImplF> OverlapWilsonContFracZolotarevFermionF;
typedef OverlapWilsonContFracZolotarevFermion<WilsonImplD> OverlapWilsonContFracZolotarevFermionD;
// Partial fraction
typedef OverlapWilsonPartialFractionTanhFermion<WilsonImplR> OverlapWilsonPartialFractionTanhFermionR;
typedef OverlapWilsonPartialFractionTanhFermion<WilsonImplF> OverlapWilsonPartialFractionTanhFermionF;
typedef OverlapWilsonPartialFractionTanhFermion<WilsonImplD> OverlapWilsonPartialFractionTanhFermionD;
typedef OverlapWilsonPartialFractionZolotarevFermion<WilsonImplR> OverlapWilsonPartialFractionZolotarevFermionR;
typedef OverlapWilsonPartialFractionZolotarevFermion<WilsonImplF> OverlapWilsonPartialFractionZolotarevFermionF;
typedef OverlapWilsonPartialFractionZolotarevFermion<WilsonImplD> OverlapWilsonPartialFractionZolotarevFermionD;
Gparity valence test now working. Interface in FermionOperator will change a lot in future
2015-08-14 00:01:04 +01:00
// Gparity cases; partial list until tested
typedef WilsonFermion<GparityWilsonImplR> GparityWilsonFermionR;
typedef WilsonFermion<GparityWilsonImplF> GparityWilsonFermionF;
typedef WilsonFermion<GparityWilsonImplD> GparityWilsonFermionD;
typedef DomainWallFermion<GparityWilsonImplR> GparityDomainWallFermionR;
typedef DomainWallFermion<GparityWilsonImplF> GparityDomainWallFermionF;
typedef DomainWallFermion<GparityWilsonImplD> GparityDomainWallFermionD;
Faiing to compile, comparing with master
2016-01-25 21:03:02 +00:00
typedef WilsonTMFermion<GparityWilsonImplR> GparityWilsonTMFermionR;
typedef WilsonTMFermion<GparityWilsonImplF> GparityWilsonTMFermionF;
typedef WilsonTMFermion<GparityWilsonImplD> GparityWilsonTMFermionD;
Added gparity mobius defs, added params to ScaledShamir checking in before puling master
2015-12-14 17:15:06 +00:00
typedef MobiusFermion<GparityWilsonImplR> GparityMobiusFermionR;
typedef MobiusFermion<GparityWilsonImplF> GparityMobiusFermionF;
typedef MobiusFermion<GparityWilsonImplD> GparityMobiusFermionD;
Merge remote-tracking branch 'origin/chulwoo-dec12-2015' Merge Chulwoo's Lanczos related improvements. Merge Nd!=4 fixes for pure gauge HMC from Evan.
2016-03-08 09:55:14 +00:00
Staggered phases first cut, c1, c2, u0
2016-11-03 16:26:56 +00:00
typedef ImprovedStaggeredFermion<StaggeredImplR> ImprovedStaggeredFermionR;
typedef ImprovedStaggeredFermion<StaggeredImplF> ImprovedStaggeredFermionF;
typedef ImprovedStaggeredFermion<StaggeredImplD> ImprovedStaggeredFermionD;
Gparity valence test now working. Interface in FermionOperator will change a lot in future
2015-08-14 00:01:04 +01:00
Staggerd Fermion 5D
2016-11-29 13:13:56 +00:00
typedef ImprovedStaggeredFermion5D<StaggeredImplR> ImprovedStaggeredFermion5DR;
typedef ImprovedStaggeredFermion5D<StaggeredImplF> ImprovedStaggeredFermion5DF;
typedef ImprovedStaggeredFermion5D<StaggeredImplD> ImprovedStaggeredFermion5DD;
Assembler possibly working
2016-12-16 16:55:36 +00:00
typedef ImprovedStaggeredFermion5D<StaggeredVec5dImplR> ImprovedStaggeredFermionVec5dR;
typedef ImprovedStaggeredFermion5D<StaggeredVec5dImplF> ImprovedStaggeredFermionVec5dF;
typedef ImprovedStaggeredFermion5D<StaggeredVec5dImplD> ImprovedStaggeredFermionVec5dD;
Gparity valence test now working. Interface in FermionOperator will change a lot in future
2015-08-14 00:01:04 +01:00
Actions updated
2016-11-29 00:14:36 +00:00
Rework/global edit to enforce type templating of fermion operators. Allows multi-precision work and paves the way for alternate BC's and such like allowing for example G-parity which is important for K pipi programme. In particular, can drive an extra flavour index into the fermion fields using template types.
2015-08-10 20:47:44 +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
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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