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Hadrons/Modules/MDistil/Distil.hpp
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Hadrons/Modules/MDistil/Distil.hpp
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/*************************************************************************************
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Grid physics library, www.github.com/paboyle/Grid
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Source file: Hadrons/Modules/MDistil/Distil.hpp
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Copyright (C) 2015-2019
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Author: Felix Erben <ferben@ed.ac.uk>
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Author: Michael Marshall <Michael.Marshall@ed.ac.uk>
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This program is free software; you can redistribute it and/or modify
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it under the terms of the GNU General Public License as published by
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the Free Software Foundation; either version 2 of the License, or
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(at your option) any later version.
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This program is distributed in the hope that it will be useful,
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but WITHOUT ANY WARRANTY; without even the implied warranty of
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MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the
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GNU General Public License for more details.
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You should have received a copy of the GNU General Public License along
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with this program; if not, write to the Free Software Foundation, Inc.,
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51 Franklin Street, Fifth Floor, Boston, MA 02110-1301 USA.
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See the full license in the file "LICENSE" in the top level distribution directory
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*************************************************************************************/
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/* END LEGAL */
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#ifndef Hadrons_MDistil_Distil_hpp_
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#define Hadrons_MDistil_Distil_hpp_
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#include <Hadrons/NamedTensor.hpp>
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#include <Hadrons/Module.hpp>
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#include <Hadrons/ModuleFactory.hpp>
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#include <Hadrons/Solver.hpp>
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#include <Hadrons/A2AVectors.hpp>
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#include <Hadrons/DilutedNoise.hpp>
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BEGIN_HADRONS_NAMESPACE
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BEGIN_MODULE_NAMESPACE(MDistil)
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/******************************************************************************
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Distillation code that is common across modules
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Documentation on how t use this code available at
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* https://aportelli.github.io/Hadrons-doc/#/mdistil *
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Notation for (stochastic) DistilParameters taken from 1104.3870:
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TI is interlaced dilution in time (corresponding to Nt = time-dimension of the lattice)
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LI is interlaced dilution in laplacian-eigenvector space (corresponding to nvec)
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SI is interlaced dilution in spin (corresponding to Ns, taken from Grid, usually Ns=4)
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This code automatically computes perambulators using exact distillation if
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* (TI,LI,SI) = (Nt,nvec,Ns) *
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In this case, nnoise=1 and Noises is set to an array of values =1 as well.
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tsrc then specifies the only timeslice on which the sources are supported.
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(( for stochastic distillation, the vaue of tsrc has no meaning in this code ))
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******************************************************************************/
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struct DistilParameters: Serializable {
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GRID_SERIALIZABLE_CLASS_MEMBERS(DistilParameters,
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int, nvec,
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int, nnoise,
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int, tsrc,
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int, TI,
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int, LI,
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int, SI )
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DistilParameters() = default;
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DistilParameters( const DistilParameters &p ) = default; // member-wise copy
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};
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/******************************************************************************
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Make a lower dimensional grid in preparation for local slice operations
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******************************************************************************/
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inline GridCartesian * MakeLowerDimGrid( GridCartesian * gridHD )
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{
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int nd{static_cast<int>(gridHD->_ndimension)};
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Coordinate latt_size = gridHD->_gdimensions;
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latt_size[nd-1] = 1;
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Coordinate simd_layout = GridDefaultSimd(nd-1, vComplex::Nsimd());
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simd_layout.push_back( 1 );
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Coordinate mpi_layout = gridHD->_processors;
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mpi_layout[nd-1] = 1;
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GridCartesian * gridLD = new GridCartesian(latt_size,simd_layout,mpi_layout,*gridHD);
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return gridLD;
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}
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/*************************************************************************************
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Rotate eigenvectors into our phase convention
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First component of first eigenvector is real and positive
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TODO: Should this be in Distil.hpp?
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*************************************************************************************/
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inline void RotateEigen(std::vector<LatticeColourVector> & evec)
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{
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ColourVector cv0;
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auto grid = evec[0].Grid();
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Coordinate siteFirst(grid->Nd(),0);
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peekSite(cv0, evec[0], siteFirst);
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Grid::Complex cplx0 = cv0()()(0);
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if( cplx0.imag() == 0 )
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std::cout << GridLogMessage << "RotateEigen() : Site 0 : " << cplx0 << " => already meets phase convention" << std::endl;
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else
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{
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const Real cplx0_mag = Grid::sqrt(cplx0.real()*cplx0.real()+cplx0.imag()*cplx0.imag());
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Grid::Complex phase{cplx0 / Grid::Complex(cplx0_mag, 0) };
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phase.imag(-phase.imag());
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#ifdef GRID_NVCC
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//const Real cplx0_mag = thrust::abs(cplx0);
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//const Grid::Complex phase = thrust::conj(cplx0 / cplx0_mag);
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const Real argphase = thrust::arg(phase);
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#else
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//const Real cplx0_mag = std::abs(cplx0);
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//const Grid::Complex phase = std::conj(cplx0 / cplx0_mag);
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const Real argphase = std::arg(phase);
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#endif
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std::cout << GridLogMessage << "RotateEigen() : Site 0 : |" << cplx0 << "|=" << cplx0_mag << " => phase=" << (argphase / 3.14159265) << " pi" << std::endl;
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{
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// TODO: Only really needed on the master slice
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for( int k = 0 ; k < evec.size() ; k++ )
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evec[k] *= phase;
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if(grid->IsBoss()){
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for( int c = 0 ; c < Nc ; c++ )
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cv0()()(c) *= phase;
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cplx0.imag(0); // This assumes phase convention is real, positive (so I get rid of rounding error)
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//pokeSite(cv0, evec[0], siteFirst);
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pokeLocalSite(cv0, evec[0], siteFirst);
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}
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}
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}
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}
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END_MODULE_NAMESPACE
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END_HADRONS_NAMESPACE
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#endif // Hadrons_MDistil_Distil_hpp_
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