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/* |
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* Copyright (c) 2005 The University of Notre Dame. All Rights Reserved. |
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* |
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* The University of Notre Dame grants you ("Licensee") a |
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* non-exclusive, royalty free, license to use, modify and |
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* redistribute this software in source and binary code form, provided |
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* that the following conditions are met: |
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* |
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* 1. Redistributions of source code must retain the above copyright |
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* notice, this list of conditions and the following disclaimer. |
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* |
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* 2. Redistributions in binary form must reproduce the above copyright |
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* notice, this list of conditions and the following disclaimer in the |
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* documentation and/or other materials provided with the |
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* distribution. |
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* |
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* This software is provided "AS IS," without a warranty of any |
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* kind. All express or implied conditions, representations and |
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* warranties, including any implied warranty of merchantability, |
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* fitness for a particular purpose or non-infringement, are hereby |
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* excluded. The University of Notre Dame and its licensors shall not |
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* be liable for any damages suffered by licensee as a result of |
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* using, modifying or distributing the software or its |
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* derivatives. In no event will the University of Notre Dame or its |
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* licensors be liable for any lost revenue, profit or data, or for |
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* direct, indirect, special, consequential, incidental or punitive |
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* damages, however caused and regardless of the theory of liability, |
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* arising out of the use of or inability to use software, even if the |
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* University of Notre Dame has been advised of the possibility of |
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* such damages. |
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* |
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* SUPPORT OPEN SCIENCE! If you use OpenMD or its source code in your |
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* research, please cite the appropriate papers when you publish your |
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* work. Good starting points are: |
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* |
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* [1] Meineke, et al., J. Comp. Chem. 26, 252-271 (2005). |
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* [2] Fennell & Gezelter, J. Chem. Phys. 124, 234104 (2006). |
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* [3] Sun, Lin & Gezelter, J. Chem. Phys. 128, 24107 (2008). |
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* [4] Kuang & Gezelter, J. Chem. Phys. 133, 164101 (2010). |
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* [5] Vardeman, Stocker & Gezelter, J. Chem. Theory Comput. 7, 834 (2011). |
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*/ |
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#include "parallel/ForceMatrixDecomposition.hpp" |
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#include "math/SquareMatrix3.hpp" |
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#include "nonbonded/NonBondedInteraction.hpp" |
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#include "brains/SnapshotManager.hpp" |
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#include "brains/PairList.hpp" |
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|
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using namespace std; |
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namespace OpenMD { |
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|
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ForceMatrixDecomposition::ForceMatrixDecomposition(SimInfo* info, InteractionManager* iMan) : ForceDecomposition(info, iMan) { |
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|
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// In a parallel computation, row and colum scans must visit all |
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// surrounding cells (not just the 14 upper triangular blocks that |
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// are used when the processor can see all pairs) |
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#ifdef IS_MPI |
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cellOffsets_.clear(); |
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cellOffsets_.push_back( Vector3i(-1,-1,-1) ); |
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cellOffsets_.push_back( Vector3i( 0,-1,-1) ); |
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cellOffsets_.push_back( Vector3i( 1,-1,-1) ); |
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cellOffsets_.push_back( Vector3i(-1, 0,-1) ); |
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cellOffsets_.push_back( Vector3i( 0, 0,-1) ); |
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cellOffsets_.push_back( Vector3i( 1, 0,-1) ); |
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cellOffsets_.push_back( Vector3i(-1, 1,-1) ); |
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cellOffsets_.push_back( Vector3i( 0, 1,-1) ); |
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cellOffsets_.push_back( Vector3i( 1, 1,-1) ); |
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cellOffsets_.push_back( Vector3i(-1,-1, 0) ); |
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cellOffsets_.push_back( Vector3i( 0,-1, 0) ); |
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cellOffsets_.push_back( Vector3i( 1,-1, 0) ); |
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cellOffsets_.push_back( Vector3i(-1, 0, 0) ); |
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cellOffsets_.push_back( Vector3i( 0, 0, 0) ); |
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cellOffsets_.push_back( Vector3i( 1, 0, 0) ); |
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cellOffsets_.push_back( Vector3i(-1, 1, 0) ); |
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cellOffsets_.push_back( Vector3i( 0, 1, 0) ); |
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cellOffsets_.push_back( Vector3i( 1, 1, 0) ); |
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cellOffsets_.push_back( Vector3i(-1,-1, 1) ); |
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cellOffsets_.push_back( Vector3i( 0,-1, 1) ); |
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cellOffsets_.push_back( Vector3i( 1,-1, 1) ); |
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cellOffsets_.push_back( Vector3i(-1, 0, 1) ); |
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cellOffsets_.push_back( Vector3i( 0, 0, 1) ); |
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cellOffsets_.push_back( Vector3i( 1, 0, 1) ); |
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cellOffsets_.push_back( Vector3i(-1, 1, 1) ); |
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cellOffsets_.push_back( Vector3i( 0, 1, 1) ); |
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cellOffsets_.push_back( Vector3i( 1, 1, 1) ); |
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#endif |
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} |
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|
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|
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/** |
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* distributeInitialData is essentially a copy of the older fortran |
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* SimulationSetup |
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*/ |
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void ForceMatrixDecomposition::distributeInitialData() { |
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snap_ = sman_->getCurrentSnapshot(); |
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storageLayout_ = sman_->getStorageLayout(); |
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ff_ = info_->getForceField(); |
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nLocal_ = snap_->getNumberOfAtoms(); |
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|
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nGroups_ = info_->getNLocalCutoffGroups(); |
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// gather the information for atomtype IDs (atids): |
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idents = info_->getIdentArray(); |
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AtomLocalToGlobal = info_->getGlobalAtomIndices(); |
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cgLocalToGlobal = info_->getGlobalGroupIndices(); |
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vector<int> globalGroupMembership = info_->getGlobalGroupMembership(); |
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|
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massFactors = info_->getMassFactors(); |
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|
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PairList* excludes = info_->getExcludedInteractions(); |
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PairList* oneTwo = info_->getOneTwoInteractions(); |
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PairList* oneThree = info_->getOneThreeInteractions(); |
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PairList* oneFour = info_->getOneFourInteractions(); |
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|
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if (needVelocities_) |
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snap_->cgData.setStorageLayout(DataStorage::dslPosition | |
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DataStorage::dslVelocity); |
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else |
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snap_->cgData.setStorageLayout(DataStorage::dslPosition); |
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|
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#ifdef IS_MPI |
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|
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MPI::Intracomm row = rowComm.getComm(); |
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MPI::Intracomm col = colComm.getComm(); |
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|
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AtomPlanIntRow = new Plan<int>(row, nLocal_); |
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AtomPlanRealRow = new Plan<RealType>(row, nLocal_); |
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AtomPlanVectorRow = new Plan<Vector3d>(row, nLocal_); |
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AtomPlanMatrixRow = new Plan<Mat3x3d>(row, nLocal_); |
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AtomPlanPotRow = new Plan<potVec>(row, nLocal_); |
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|
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AtomPlanIntColumn = new Plan<int>(col, nLocal_); |
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AtomPlanRealColumn = new Plan<RealType>(col, nLocal_); |
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AtomPlanVectorColumn = new Plan<Vector3d>(col, nLocal_); |
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AtomPlanMatrixColumn = new Plan<Mat3x3d>(col, nLocal_); |
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AtomPlanPotColumn = new Plan<potVec>(col, nLocal_); |
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|
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cgPlanIntRow = new Plan<int>(row, nGroups_); |
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cgPlanVectorRow = new Plan<Vector3d>(row, nGroups_); |
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cgPlanIntColumn = new Plan<int>(col, nGroups_); |
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cgPlanVectorColumn = new Plan<Vector3d>(col, nGroups_); |
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|
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nAtomsInRow_ = AtomPlanIntRow->getSize(); |
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nAtomsInCol_ = AtomPlanIntColumn->getSize(); |
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nGroupsInRow_ = cgPlanIntRow->getSize(); |
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nGroupsInCol_ = cgPlanIntColumn->getSize(); |
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|
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// Modify the data storage objects with the correct layouts and sizes: |
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atomRowData.resize(nAtomsInRow_); |
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atomRowData.setStorageLayout(storageLayout_); |
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atomColData.resize(nAtomsInCol_); |
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atomColData.setStorageLayout(storageLayout_); |
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cgRowData.resize(nGroupsInRow_); |
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cgRowData.setStorageLayout(DataStorage::dslPosition); |
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cgColData.resize(nGroupsInCol_); |
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if (needVelocities_) |
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// we only need column velocities if we need them. |
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cgColData.setStorageLayout(DataStorage::dslPosition | |
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DataStorage::dslVelocity); |
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else |
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cgColData.setStorageLayout(DataStorage::dslPosition); |
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|
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identsRow.resize(nAtomsInRow_); |
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identsCol.resize(nAtomsInCol_); |
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|
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AtomPlanIntRow->gather(idents, identsRow); |
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AtomPlanIntColumn->gather(idents, identsCol); |
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|
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// allocate memory for the parallel objects |
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atypesRow.resize(nAtomsInRow_); |
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atypesCol.resize(nAtomsInCol_); |
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|
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for (int i = 0; i < nAtomsInRow_; i++) |
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atypesRow[i] = ff_->getAtomType(identsRow[i]); |
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for (int i = 0; i < nAtomsInCol_; i++) |
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atypesCol[i] = ff_->getAtomType(identsCol[i]); |
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|
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pot_row.resize(nAtomsInRow_); |
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pot_col.resize(nAtomsInCol_); |
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|
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expot_row.resize(nAtomsInRow_); |
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expot_col.resize(nAtomsInCol_); |
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|
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AtomRowToGlobal.resize(nAtomsInRow_); |
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AtomColToGlobal.resize(nAtomsInCol_); |
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AtomPlanIntRow->gather(AtomLocalToGlobal, AtomRowToGlobal); |
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AtomPlanIntColumn->gather(AtomLocalToGlobal, AtomColToGlobal); |
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|
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cgRowToGlobal.resize(nGroupsInRow_); |
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cgColToGlobal.resize(nGroupsInCol_); |
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cgPlanIntRow->gather(cgLocalToGlobal, cgRowToGlobal); |
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cgPlanIntColumn->gather(cgLocalToGlobal, cgColToGlobal); |
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|
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massFactorsRow.resize(nAtomsInRow_); |
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massFactorsCol.resize(nAtomsInCol_); |
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AtomPlanRealRow->gather(massFactors, massFactorsRow); |
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AtomPlanRealColumn->gather(massFactors, massFactorsCol); |
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|
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groupListRow_.clear(); |
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groupListRow_.resize(nGroupsInRow_); |
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for (int i = 0; i < nGroupsInRow_; i++) { |
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int gid = cgRowToGlobal[i]; |
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for (int j = 0; j < nAtomsInRow_; j++) { |
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int aid = AtomRowToGlobal[j]; |
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if (globalGroupMembership[aid] == gid) |
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groupListRow_[i].push_back(j); |
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} |
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} |
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|
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groupListCol_.clear(); |
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groupListCol_.resize(nGroupsInCol_); |
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for (int i = 0; i < nGroupsInCol_; i++) { |
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int gid = cgColToGlobal[i]; |
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for (int j = 0; j < nAtomsInCol_; j++) { |
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int aid = AtomColToGlobal[j]; |
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if (globalGroupMembership[aid] == gid) |
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groupListCol_[i].push_back(j); |
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} |
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} |
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|
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excludesForAtom.clear(); |
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excludesForAtom.resize(nAtomsInRow_); |
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toposForAtom.clear(); |
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toposForAtom.resize(nAtomsInRow_); |
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topoDist.clear(); |
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topoDist.resize(nAtomsInRow_); |
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for (int i = 0; i < nAtomsInRow_; i++) { |
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int iglob = AtomRowToGlobal[i]; |
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|
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for (int j = 0; j < nAtomsInCol_; j++) { |
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int jglob = AtomColToGlobal[j]; |
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|
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if (excludes->hasPair(iglob, jglob)) |
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excludesForAtom[i].push_back(j); |
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|
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if (oneTwo->hasPair(iglob, jglob)) { |
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toposForAtom[i].push_back(j); |
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topoDist[i].push_back(1); |
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} else { |
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if (oneThree->hasPair(iglob, jglob)) { |
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toposForAtom[i].push_back(j); |
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topoDist[i].push_back(2); |
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} else { |
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if (oneFour->hasPair(iglob, jglob)) { |
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toposForAtom[i].push_back(j); |
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topoDist[i].push_back(3); |
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} |
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} |
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} |
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} |
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} |
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|
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#else |
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excludesForAtom.clear(); |
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excludesForAtom.resize(nLocal_); |
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toposForAtom.clear(); |
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toposForAtom.resize(nLocal_); |
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topoDist.clear(); |
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topoDist.resize(nLocal_); |
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|
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for (int i = 0; i < nLocal_; i++) { |
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int iglob = AtomLocalToGlobal[i]; |
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|
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for (int j = 0; j < nLocal_; j++) { |
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int jglob = AtomLocalToGlobal[j]; |
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|
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if (excludes->hasPair(iglob, jglob)) |
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excludesForAtom[i].push_back(j); |
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|
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if (oneTwo->hasPair(iglob, jglob)) { |
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toposForAtom[i].push_back(j); |
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topoDist[i].push_back(1); |
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} else { |
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if (oneThree->hasPair(iglob, jglob)) { |
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toposForAtom[i].push_back(j); |
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topoDist[i].push_back(2); |
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} else { |
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if (oneFour->hasPair(iglob, jglob)) { |
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toposForAtom[i].push_back(j); |
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topoDist[i].push_back(3); |
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} |
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} |
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} |
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} |
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} |
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#endif |
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|
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// allocate memory for the parallel objects |
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atypesLocal.resize(nLocal_); |
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|
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for (int i = 0; i < nLocal_; i++) |
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atypesLocal[i] = ff_->getAtomType(idents[i]); |
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|
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groupList_.clear(); |
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groupList_.resize(nGroups_); |
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for (int i = 0; i < nGroups_; i++) { |
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int gid = cgLocalToGlobal[i]; |
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for (int j = 0; j < nLocal_; j++) { |
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int aid = AtomLocalToGlobal[j]; |
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if (globalGroupMembership[aid] == gid) { |
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groupList_[i].push_back(j); |
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} |
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} |
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} |
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|
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|
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createGtypeCutoffMap(); |
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|
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} |
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|
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void ForceMatrixDecomposition::createGtypeCutoffMap() { |
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|
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RealType tol = 1e-6; |
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largestRcut_ = 0.0; |
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RealType rc; |
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int atid; |
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set<AtomType*> atypes = info_->getSimulatedAtomTypes(); |
316 |
|
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map<int, RealType> atypeCutoff; |
318 |
|
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for (set<AtomType*>::iterator at = atypes.begin(); |
320 |
at != atypes.end(); ++at){ |
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atid = (*at)->getIdent(); |
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if (userChoseCutoff_) |
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atypeCutoff[atid] = userCutoff_; |
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else |
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atypeCutoff[atid] = interactionMan_->getSuggestedCutoffRadius(*at); |
326 |
} |
327 |
|
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vector<RealType> gTypeCutoffs; |
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// first we do a single loop over the cutoff groups to find the |
330 |
// largest cutoff for any atypes present in this group. |
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#ifdef IS_MPI |
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vector<RealType> groupCutoffRow(nGroupsInRow_, 0.0); |
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groupRowToGtype.resize(nGroupsInRow_); |
334 |
for (int cg1 = 0; cg1 < nGroupsInRow_; cg1++) { |
335 |
vector<int> atomListRow = getAtomsInGroupRow(cg1); |
336 |
for (vector<int>::iterator ia = atomListRow.begin(); |
337 |
ia != atomListRow.end(); ++ia) { |
338 |
int atom1 = (*ia); |
339 |
atid = identsRow[atom1]; |
340 |
if (atypeCutoff[atid] > groupCutoffRow[cg1]) { |
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groupCutoffRow[cg1] = atypeCutoff[atid]; |
342 |
} |
343 |
} |
344 |
|
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bool gTypeFound = false; |
346 |
for (int gt = 0; gt < gTypeCutoffs.size(); gt++) { |
347 |
if (abs(groupCutoffRow[cg1] - gTypeCutoffs[gt]) < tol) { |
348 |
groupRowToGtype[cg1] = gt; |
349 |
gTypeFound = true; |
350 |
} |
351 |
} |
352 |
if (!gTypeFound) { |
353 |
gTypeCutoffs.push_back( groupCutoffRow[cg1] ); |
354 |
groupRowToGtype[cg1] = gTypeCutoffs.size() - 1; |
355 |
} |
356 |
|
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} |
358 |
vector<RealType> groupCutoffCol(nGroupsInCol_, 0.0); |
359 |
groupColToGtype.resize(nGroupsInCol_); |
360 |
for (int cg2 = 0; cg2 < nGroupsInCol_; cg2++) { |
361 |
vector<int> atomListCol = getAtomsInGroupColumn(cg2); |
362 |
for (vector<int>::iterator jb = atomListCol.begin(); |
363 |
jb != atomListCol.end(); ++jb) { |
364 |
int atom2 = (*jb); |
365 |
atid = identsCol[atom2]; |
366 |
if (atypeCutoff[atid] > groupCutoffCol[cg2]) { |
367 |
groupCutoffCol[cg2] = atypeCutoff[atid]; |
368 |
} |
369 |
} |
370 |
bool gTypeFound = false; |
371 |
for (int gt = 0; gt < gTypeCutoffs.size(); gt++) { |
372 |
if (abs(groupCutoffCol[cg2] - gTypeCutoffs[gt]) < tol) { |
373 |
groupColToGtype[cg2] = gt; |
374 |
gTypeFound = true; |
375 |
} |
376 |
} |
377 |
if (!gTypeFound) { |
378 |
gTypeCutoffs.push_back( groupCutoffCol[cg2] ); |
379 |
groupColToGtype[cg2] = gTypeCutoffs.size() - 1; |
380 |
} |
381 |
} |
382 |
#else |
383 |
|
384 |
vector<RealType> groupCutoff(nGroups_, 0.0); |
385 |
groupToGtype.resize(nGroups_); |
386 |
for (int cg1 = 0; cg1 < nGroups_; cg1++) { |
387 |
groupCutoff[cg1] = 0.0; |
388 |
vector<int> atomList = getAtomsInGroupRow(cg1); |
389 |
for (vector<int>::iterator ia = atomList.begin(); |
390 |
ia != atomList.end(); ++ia) { |
391 |
int atom1 = (*ia); |
392 |
atid = idents[atom1]; |
393 |
if (atypeCutoff[atid] > groupCutoff[cg1]) |
394 |
groupCutoff[cg1] = atypeCutoff[atid]; |
395 |
} |
396 |
|
397 |
bool gTypeFound = false; |
398 |
for (int gt = 0; gt < gTypeCutoffs.size(); gt++) { |
399 |
if (abs(groupCutoff[cg1] - gTypeCutoffs[gt]) < tol) { |
400 |
groupToGtype[cg1] = gt; |
401 |
gTypeFound = true; |
402 |
} |
403 |
} |
404 |
if (!gTypeFound) { |
405 |
gTypeCutoffs.push_back( groupCutoff[cg1] ); |
406 |
groupToGtype[cg1] = gTypeCutoffs.size() - 1; |
407 |
} |
408 |
} |
409 |
#endif |
410 |
|
411 |
// Now we find the maximum group cutoff value present in the simulation |
412 |
|
413 |
RealType groupMax = *max_element(gTypeCutoffs.begin(), |
414 |
gTypeCutoffs.end()); |
415 |
|
416 |
#ifdef IS_MPI |
417 |
MPI::COMM_WORLD.Allreduce(&groupMax, &groupMax, 1, MPI::REALTYPE, |
418 |
MPI::MAX); |
419 |
#endif |
420 |
|
421 |
RealType tradRcut = groupMax; |
422 |
|
423 |
for (int i = 0; i < gTypeCutoffs.size(); i++) { |
424 |
for (int j = 0; j < gTypeCutoffs.size(); j++) { |
425 |
RealType thisRcut; |
426 |
switch(cutoffPolicy_) { |
427 |
case TRADITIONAL: |
428 |
thisRcut = tradRcut; |
429 |
break; |
430 |
case MIX: |
431 |
thisRcut = 0.5 * (gTypeCutoffs[i] + gTypeCutoffs[j]); |
432 |
break; |
433 |
case MAX: |
434 |
thisRcut = max(gTypeCutoffs[i], gTypeCutoffs[j]); |
435 |
break; |
436 |
default: |
437 |
sprintf(painCave.errMsg, |
438 |
"ForceMatrixDecomposition::createGtypeCutoffMap " |
439 |
"hit an unknown cutoff policy!\n"); |
440 |
painCave.severity = OPENMD_ERROR; |
441 |
painCave.isFatal = 1; |
442 |
simError(); |
443 |
break; |
444 |
} |
445 |
|
446 |
pair<int,int> key = make_pair(i,j); |
447 |
gTypeCutoffMap[key].first = thisRcut; |
448 |
if (thisRcut > largestRcut_) largestRcut_ = thisRcut; |
449 |
gTypeCutoffMap[key].second = thisRcut*thisRcut; |
450 |
gTypeCutoffMap[key].third = pow(thisRcut + skinThickness_, 2); |
451 |
// sanity check |
452 |
|
453 |
if (userChoseCutoff_) { |
454 |
if (abs(gTypeCutoffMap[key].first - userCutoff_) > 0.0001) { |
455 |
sprintf(painCave.errMsg, |
456 |
"ForceMatrixDecomposition::createGtypeCutoffMap " |
457 |
"user-specified rCut (%lf) does not match computed group Cutoff\n", userCutoff_); |
458 |
painCave.severity = OPENMD_ERROR; |
459 |
painCave.isFatal = 1; |
460 |
simError(); |
461 |
} |
462 |
} |
463 |
} |
464 |
} |
465 |
} |
466 |
|
467 |
groupCutoffs ForceMatrixDecomposition::getGroupCutoffs(int cg1, int cg2) { |
468 |
int i, j; |
469 |
#ifdef IS_MPI |
470 |
i = groupRowToGtype[cg1]; |
471 |
j = groupColToGtype[cg2]; |
472 |
#else |
473 |
i = groupToGtype[cg1]; |
474 |
j = groupToGtype[cg2]; |
475 |
#endif |
476 |
return gTypeCutoffMap[make_pair(i,j)]; |
477 |
} |
478 |
|
479 |
int ForceMatrixDecomposition::getTopologicalDistance(int atom1, int atom2) { |
480 |
for (int j = 0; j < toposForAtom[atom1].size(); j++) { |
481 |
if (toposForAtom[atom1][j] == atom2) |
482 |
return topoDist[atom1][j]; |
483 |
} |
484 |
return 0; |
485 |
} |
486 |
|
487 |
void ForceMatrixDecomposition::zeroWorkArrays() { |
488 |
pairwisePot = 0.0; |
489 |
embeddingPot = 0.0; |
490 |
excludedPot = 0.0; |
491 |
|
492 |
#ifdef IS_MPI |
493 |
if (storageLayout_ & DataStorage::dslForce) { |
494 |
fill(atomRowData.force.begin(), atomRowData.force.end(), V3Zero); |
495 |
fill(atomColData.force.begin(), atomColData.force.end(), V3Zero); |
496 |
} |
497 |
|
498 |
if (storageLayout_ & DataStorage::dslTorque) { |
499 |
fill(atomRowData.torque.begin(), atomRowData.torque.end(), V3Zero); |
500 |
fill(atomColData.torque.begin(), atomColData.torque.end(), V3Zero); |
501 |
} |
502 |
|
503 |
fill(pot_row.begin(), pot_row.end(), |
504 |
Vector<RealType, N_INTERACTION_FAMILIES> (0.0)); |
505 |
|
506 |
fill(pot_col.begin(), pot_col.end(), |
507 |
Vector<RealType, N_INTERACTION_FAMILIES> (0.0)); |
508 |
|
509 |
fill(expot_row.begin(), expot_row.end(), |
510 |
Vector<RealType, N_INTERACTION_FAMILIES> (0.0)); |
511 |
|
512 |
fill(expot_col.begin(), expot_col.end(), |
513 |
Vector<RealType, N_INTERACTION_FAMILIES> (0.0)); |
514 |
|
515 |
if (storageLayout_ & DataStorage::dslParticlePot) { |
516 |
fill(atomRowData.particlePot.begin(), atomRowData.particlePot.end(), |
517 |
0.0); |
518 |
fill(atomColData.particlePot.begin(), atomColData.particlePot.end(), |
519 |
0.0); |
520 |
} |
521 |
|
522 |
if (storageLayout_ & DataStorage::dslDensity) { |
523 |
fill(atomRowData.density.begin(), atomRowData.density.end(), 0.0); |
524 |
fill(atomColData.density.begin(), atomColData.density.end(), 0.0); |
525 |
} |
526 |
|
527 |
if (storageLayout_ & DataStorage::dslFunctional) { |
528 |
fill(atomRowData.functional.begin(), atomRowData.functional.end(), |
529 |
0.0); |
530 |
fill(atomColData.functional.begin(), atomColData.functional.end(), |
531 |
0.0); |
532 |
} |
533 |
|
534 |
if (storageLayout_ & DataStorage::dslFunctionalDerivative) { |
535 |
fill(atomRowData.functionalDerivative.begin(), |
536 |
atomRowData.functionalDerivative.end(), 0.0); |
537 |
fill(atomColData.functionalDerivative.begin(), |
538 |
atomColData.functionalDerivative.end(), 0.0); |
539 |
} |
540 |
|
541 |
if (storageLayout_ & DataStorage::dslSkippedCharge) { |
542 |
fill(atomRowData.skippedCharge.begin(), |
543 |
atomRowData.skippedCharge.end(), 0.0); |
544 |
fill(atomColData.skippedCharge.begin(), |
545 |
atomColData.skippedCharge.end(), 0.0); |
546 |
} |
547 |
|
548 |
if (storageLayout_ & DataStorage::dslFlucQForce) { |
549 |
fill(atomRowData.flucQFrc.begin(), |
550 |
atomRowData.flucQFrc.end(), 0.0); |
551 |
fill(atomColData.flucQFrc.begin(), |
552 |
atomColData.flucQFrc.end(), 0.0); |
553 |
} |
554 |
|
555 |
if (storageLayout_ & DataStorage::dslElectricField) { |
556 |
fill(atomRowData.electricField.begin(), |
557 |
atomRowData.electricField.end(), V3Zero); |
558 |
fill(atomColData.electricField.begin(), |
559 |
atomColData.electricField.end(), V3Zero); |
560 |
} |
561 |
|
562 |
if (storageLayout_ & DataStorage::dslFlucQForce) { |
563 |
fill(atomRowData.flucQFrc.begin(), atomRowData.flucQFrc.end(), |
564 |
0.0); |
565 |
fill(atomColData.flucQFrc.begin(), atomColData.flucQFrc.end(), |
566 |
0.0); |
567 |
} |
568 |
|
569 |
#endif |
570 |
// even in parallel, we need to zero out the local arrays: |
571 |
|
572 |
if (storageLayout_ & DataStorage::dslParticlePot) { |
573 |
fill(snap_->atomData.particlePot.begin(), |
574 |
snap_->atomData.particlePot.end(), 0.0); |
575 |
} |
576 |
|
577 |
if (storageLayout_ & DataStorage::dslDensity) { |
578 |
fill(snap_->atomData.density.begin(), |
579 |
snap_->atomData.density.end(), 0.0); |
580 |
} |
581 |
|
582 |
if (storageLayout_ & DataStorage::dslFunctional) { |
583 |
fill(snap_->atomData.functional.begin(), |
584 |
snap_->atomData.functional.end(), 0.0); |
585 |
} |
586 |
|
587 |
if (storageLayout_ & DataStorage::dslFunctionalDerivative) { |
588 |
fill(snap_->atomData.functionalDerivative.begin(), |
589 |
snap_->atomData.functionalDerivative.end(), 0.0); |
590 |
} |
591 |
|
592 |
if (storageLayout_ & DataStorage::dslSkippedCharge) { |
593 |
fill(snap_->atomData.skippedCharge.begin(), |
594 |
snap_->atomData.skippedCharge.end(), 0.0); |
595 |
} |
596 |
|
597 |
if (storageLayout_ & DataStorage::dslElectricField) { |
598 |
fill(snap_->atomData.electricField.begin(), |
599 |
snap_->atomData.electricField.end(), V3Zero); |
600 |
} |
601 |
} |
602 |
|
603 |
|
604 |
void ForceMatrixDecomposition::distributeData() { |
605 |
snap_ = sman_->getCurrentSnapshot(); |
606 |
storageLayout_ = sman_->getStorageLayout(); |
607 |
#ifdef IS_MPI |
608 |
|
609 |
// gather up the atomic positions |
610 |
AtomPlanVectorRow->gather(snap_->atomData.position, |
611 |
atomRowData.position); |
612 |
AtomPlanVectorColumn->gather(snap_->atomData.position, |
613 |
atomColData.position); |
614 |
|
615 |
// gather up the cutoff group positions |
616 |
|
617 |
cgPlanVectorRow->gather(snap_->cgData.position, |
618 |
cgRowData.position); |
619 |
|
620 |
cgPlanVectorColumn->gather(snap_->cgData.position, |
621 |
cgColData.position); |
622 |
|
623 |
|
624 |
|
625 |
if (needVelocities_) { |
626 |
// gather up the atomic velocities |
627 |
AtomPlanVectorColumn->gather(snap_->atomData.velocity, |
628 |
atomColData.velocity); |
629 |
|
630 |
cgPlanVectorColumn->gather(snap_->cgData.velocity, |
631 |
cgColData.velocity); |
632 |
} |
633 |
|
634 |
|
635 |
// if needed, gather the atomic rotation matrices |
636 |
if (storageLayout_ & DataStorage::dslAmat) { |
637 |
AtomPlanMatrixRow->gather(snap_->atomData.aMat, |
638 |
atomRowData.aMat); |
639 |
AtomPlanMatrixColumn->gather(snap_->atomData.aMat, |
640 |
atomColData.aMat); |
641 |
} |
642 |
|
643 |
// if needed, gather the atomic eletrostatic frames |
644 |
if (storageLayout_ & DataStorage::dslElectroFrame) { |
645 |
AtomPlanMatrixRow->gather(snap_->atomData.electroFrame, |
646 |
atomRowData.electroFrame); |
647 |
AtomPlanMatrixColumn->gather(snap_->atomData.electroFrame, |
648 |
atomColData.electroFrame); |
649 |
} |
650 |
|
651 |
// if needed, gather the atomic fluctuating charge values |
652 |
if (storageLayout_ & DataStorage::dslFlucQPosition) { |
653 |
AtomPlanRealRow->gather(snap_->atomData.flucQPos, |
654 |
atomRowData.flucQPos); |
655 |
AtomPlanRealColumn->gather(snap_->atomData.flucQPos, |
656 |
atomColData.flucQPos); |
657 |
} |
658 |
|
659 |
#endif |
660 |
} |
661 |
|
662 |
/* collects information obtained during the pre-pair loop onto local |
663 |
* data structures. |
664 |
*/ |
665 |
void ForceMatrixDecomposition::collectIntermediateData() { |
666 |
snap_ = sman_->getCurrentSnapshot(); |
667 |
storageLayout_ = sman_->getStorageLayout(); |
668 |
#ifdef IS_MPI |
669 |
|
670 |
if (storageLayout_ & DataStorage::dslDensity) { |
671 |
|
672 |
AtomPlanRealRow->scatter(atomRowData.density, |
673 |
snap_->atomData.density); |
674 |
|
675 |
int n = snap_->atomData.density.size(); |
676 |
vector<RealType> rho_tmp(n, 0.0); |
677 |
AtomPlanRealColumn->scatter(atomColData.density, rho_tmp); |
678 |
for (int i = 0; i < n; i++) |
679 |
snap_->atomData.density[i] += rho_tmp[i]; |
680 |
} |
681 |
|
682 |
if (storageLayout_ & DataStorage::dslElectricField) { |
683 |
|
684 |
AtomPlanVectorRow->scatter(atomRowData.electricField, |
685 |
snap_->atomData.electricField); |
686 |
|
687 |
int n = snap_->atomData.electricField.size(); |
688 |
vector<Vector3d> field_tmp(n, V3Zero); |
689 |
AtomPlanVectorColumn->scatter(atomColData.electricField, field_tmp); |
690 |
for (int i = 0; i < n; i++) |
691 |
snap_->atomData.electricField[i] += field_tmp[i]; |
692 |
} |
693 |
#endif |
694 |
} |
695 |
|
696 |
/* |
697 |
* redistributes information obtained during the pre-pair loop out to |
698 |
* row and column-indexed data structures |
699 |
*/ |
700 |
void ForceMatrixDecomposition::distributeIntermediateData() { |
701 |
snap_ = sman_->getCurrentSnapshot(); |
702 |
storageLayout_ = sman_->getStorageLayout(); |
703 |
#ifdef IS_MPI |
704 |
if (storageLayout_ & DataStorage::dslFunctional) { |
705 |
AtomPlanRealRow->gather(snap_->atomData.functional, |
706 |
atomRowData.functional); |
707 |
AtomPlanRealColumn->gather(snap_->atomData.functional, |
708 |
atomColData.functional); |
709 |
} |
710 |
|
711 |
if (storageLayout_ & DataStorage::dslFunctionalDerivative) { |
712 |
AtomPlanRealRow->gather(snap_->atomData.functionalDerivative, |
713 |
atomRowData.functionalDerivative); |
714 |
AtomPlanRealColumn->gather(snap_->atomData.functionalDerivative, |
715 |
atomColData.functionalDerivative); |
716 |
} |
717 |
#endif |
718 |
} |
719 |
|
720 |
|
721 |
void ForceMatrixDecomposition::collectData() { |
722 |
snap_ = sman_->getCurrentSnapshot(); |
723 |
storageLayout_ = sman_->getStorageLayout(); |
724 |
#ifdef IS_MPI |
725 |
int n = snap_->atomData.force.size(); |
726 |
vector<Vector3d> frc_tmp(n, V3Zero); |
727 |
|
728 |
AtomPlanVectorRow->scatter(atomRowData.force, frc_tmp); |
729 |
for (int i = 0; i < n; i++) { |
730 |
snap_->atomData.force[i] += frc_tmp[i]; |
731 |
frc_tmp[i] = 0.0; |
732 |
} |
733 |
|
734 |
AtomPlanVectorColumn->scatter(atomColData.force, frc_tmp); |
735 |
for (int i = 0; i < n; i++) { |
736 |
snap_->atomData.force[i] += frc_tmp[i]; |
737 |
} |
738 |
|
739 |
if (storageLayout_ & DataStorage::dslTorque) { |
740 |
|
741 |
int nt = snap_->atomData.torque.size(); |
742 |
vector<Vector3d> trq_tmp(nt, V3Zero); |
743 |
|
744 |
AtomPlanVectorRow->scatter(atomRowData.torque, trq_tmp); |
745 |
for (int i = 0; i < nt; i++) { |
746 |
snap_->atomData.torque[i] += trq_tmp[i]; |
747 |
trq_tmp[i] = 0.0; |
748 |
} |
749 |
|
750 |
AtomPlanVectorColumn->scatter(atomColData.torque, trq_tmp); |
751 |
for (int i = 0; i < nt; i++) |
752 |
snap_->atomData.torque[i] += trq_tmp[i]; |
753 |
} |
754 |
|
755 |
if (storageLayout_ & DataStorage::dslSkippedCharge) { |
756 |
|
757 |
int ns = snap_->atomData.skippedCharge.size(); |
758 |
vector<RealType> skch_tmp(ns, 0.0); |
759 |
|
760 |
AtomPlanRealRow->scatter(atomRowData.skippedCharge, skch_tmp); |
761 |
for (int i = 0; i < ns; i++) { |
762 |
snap_->atomData.skippedCharge[i] += skch_tmp[i]; |
763 |
skch_tmp[i] = 0.0; |
764 |
} |
765 |
|
766 |
AtomPlanRealColumn->scatter(atomColData.skippedCharge, skch_tmp); |
767 |
for (int i = 0; i < ns; i++) |
768 |
snap_->atomData.skippedCharge[i] += skch_tmp[i]; |
769 |
|
770 |
} |
771 |
|
772 |
if (storageLayout_ & DataStorage::dslFlucQForce) { |
773 |
|
774 |
int nq = snap_->atomData.flucQFrc.size(); |
775 |
vector<RealType> fqfrc_tmp(nq, 0.0); |
776 |
|
777 |
AtomPlanRealRow->scatter(atomRowData.flucQFrc, fqfrc_tmp); |
778 |
for (int i = 0; i < nq; i++) { |
779 |
snap_->atomData.flucQFrc[i] += fqfrc_tmp[i]; |
780 |
fqfrc_tmp[i] = 0.0; |
781 |
} |
782 |
|
783 |
AtomPlanRealColumn->scatter(atomColData.flucQFrc, fqfrc_tmp); |
784 |
for (int i = 0; i < nq; i++) |
785 |
snap_->atomData.flucQFrc[i] += fqfrc_tmp[i]; |
786 |
|
787 |
} |
788 |
|
789 |
nLocal_ = snap_->getNumberOfAtoms(); |
790 |
|
791 |
vector<potVec> pot_temp(nLocal_, |
792 |
Vector<RealType, N_INTERACTION_FAMILIES> (0.0)); |
793 |
vector<potVec> expot_temp(nLocal_, |
794 |
Vector<RealType, N_INTERACTION_FAMILIES> (0.0)); |
795 |
|
796 |
// scatter/gather pot_row into the members of my column |
797 |
|
798 |
AtomPlanPotRow->scatter(pot_row, pot_temp); |
799 |
AtomPlanPotRow->scatter(expot_row, expot_temp); |
800 |
|
801 |
for (int ii = 0; ii < pot_temp.size(); ii++ ) |
802 |
pairwisePot += pot_temp[ii]; |
803 |
|
804 |
for (int ii = 0; ii < expot_temp.size(); ii++ ) |
805 |
excludedPot += expot_temp[ii]; |
806 |
|
807 |
if (storageLayout_ & DataStorage::dslParticlePot) { |
808 |
// This is the pairwise contribution to the particle pot. The |
809 |
// embedding contribution is added in each of the low level |
810 |
// non-bonded routines. In single processor, this is done in |
811 |
// unpackInteractionData, not in collectData. |
812 |
for (int ii = 0; ii < N_INTERACTION_FAMILIES; ii++) { |
813 |
for (int i = 0; i < nLocal_; i++) { |
814 |
// factor of two is because the total potential terms are divided |
815 |
// by 2 in parallel due to row/ column scatter |
816 |
snap_->atomData.particlePot[i] += 2.0 * pot_temp[i](ii); |
817 |
} |
818 |
} |
819 |
} |
820 |
|
821 |
fill(pot_temp.begin(), pot_temp.end(), |
822 |
Vector<RealType, N_INTERACTION_FAMILIES> (0.0)); |
823 |
fill(expot_temp.begin(), expot_temp.end(), |
824 |
Vector<RealType, N_INTERACTION_FAMILIES> (0.0)); |
825 |
|
826 |
AtomPlanPotColumn->scatter(pot_col, pot_temp); |
827 |
AtomPlanPotColumn->scatter(expot_col, expot_temp); |
828 |
|
829 |
for (int ii = 0; ii < pot_temp.size(); ii++ ) |
830 |
pairwisePot += pot_temp[ii]; |
831 |
|
832 |
for (int ii = 0; ii < expot_temp.size(); ii++ ) |
833 |
excludedPot += expot_temp[ii]; |
834 |
|
835 |
if (storageLayout_ & DataStorage::dslParticlePot) { |
836 |
// This is the pairwise contribution to the particle pot. The |
837 |
// embedding contribution is added in each of the low level |
838 |
// non-bonded routines. In single processor, this is done in |
839 |
// unpackInteractionData, not in collectData. |
840 |
for (int ii = 0; ii < N_INTERACTION_FAMILIES; ii++) { |
841 |
for (int i = 0; i < nLocal_; i++) { |
842 |
// factor of two is because the total potential terms are divided |
843 |
// by 2 in parallel due to row/ column scatter |
844 |
snap_->atomData.particlePot[i] += 2.0 * pot_temp[i](ii); |
845 |
} |
846 |
} |
847 |
} |
848 |
|
849 |
if (storageLayout_ & DataStorage::dslParticlePot) { |
850 |
int npp = snap_->atomData.particlePot.size(); |
851 |
vector<RealType> ppot_temp(npp, 0.0); |
852 |
|
853 |
// This is the direct or embedding contribution to the particle |
854 |
// pot. |
855 |
|
856 |
AtomPlanRealRow->scatter(atomRowData.particlePot, ppot_temp); |
857 |
for (int i = 0; i < npp; i++) { |
858 |
snap_->atomData.particlePot[i] += ppot_temp[i]; |
859 |
} |
860 |
|
861 |
fill(ppot_temp.begin(), ppot_temp.end(), 0.0); |
862 |
|
863 |
AtomPlanRealColumn->scatter(atomColData.particlePot, ppot_temp); |
864 |
for (int i = 0; i < npp; i++) { |
865 |
snap_->atomData.particlePot[i] += ppot_temp[i]; |
866 |
} |
867 |
} |
868 |
|
869 |
for (int ii = 0; ii < N_INTERACTION_FAMILIES; ii++) { |
870 |
RealType ploc1 = pairwisePot[ii]; |
871 |
RealType ploc2 = 0.0; |
872 |
MPI::COMM_WORLD.Allreduce(&ploc1, &ploc2, 1, MPI::REALTYPE, MPI::SUM); |
873 |
pairwisePot[ii] = ploc2; |
874 |
} |
875 |
|
876 |
for (int ii = 0; ii < N_INTERACTION_FAMILIES; ii++) { |
877 |
RealType ploc1 = excludedPot[ii]; |
878 |
RealType ploc2 = 0.0; |
879 |
MPI::COMM_WORLD.Allreduce(&ploc1, &ploc2, 1, MPI::REALTYPE, MPI::SUM); |
880 |
excludedPot[ii] = ploc2; |
881 |
} |
882 |
|
883 |
// Here be dragons. |
884 |
MPI::Intracomm col = colComm.getComm(); |
885 |
|
886 |
col.Allreduce(MPI::IN_PLACE, |
887 |
&snap_->frameData.conductiveHeatFlux[0], 3, |
888 |
MPI::REALTYPE, MPI::SUM); |
889 |
|
890 |
|
891 |
#endif |
892 |
|
893 |
} |
894 |
|
895 |
/** |
896 |
* Collects information obtained during the post-pair (and embedding |
897 |
* functional) loops onto local data structures. |
898 |
*/ |
899 |
void ForceMatrixDecomposition::collectSelfData() { |
900 |
snap_ = sman_->getCurrentSnapshot(); |
901 |
storageLayout_ = sman_->getStorageLayout(); |
902 |
|
903 |
#ifdef IS_MPI |
904 |
for (int ii = 0; ii < N_INTERACTION_FAMILIES; ii++) { |
905 |
RealType ploc1 = embeddingPot[ii]; |
906 |
RealType ploc2 = 0.0; |
907 |
MPI::COMM_WORLD.Allreduce(&ploc1, &ploc2, 1, MPI::REALTYPE, MPI::SUM); |
908 |
embeddingPot[ii] = ploc2; |
909 |
} |
910 |
#endif |
911 |
|
912 |
} |
913 |
|
914 |
|
915 |
|
916 |
int ForceMatrixDecomposition::getNAtomsInRow() { |
917 |
#ifdef IS_MPI |
918 |
return nAtomsInRow_; |
919 |
#else |
920 |
return nLocal_; |
921 |
#endif |
922 |
} |
923 |
|
924 |
/** |
925 |
* returns the list of atoms belonging to this group. |
926 |
*/ |
927 |
vector<int> ForceMatrixDecomposition::getAtomsInGroupRow(int cg1){ |
928 |
#ifdef IS_MPI |
929 |
return groupListRow_[cg1]; |
930 |
#else |
931 |
return groupList_[cg1]; |
932 |
#endif |
933 |
} |
934 |
|
935 |
vector<int> ForceMatrixDecomposition::getAtomsInGroupColumn(int cg2){ |
936 |
#ifdef IS_MPI |
937 |
return groupListCol_[cg2]; |
938 |
#else |
939 |
return groupList_[cg2]; |
940 |
#endif |
941 |
} |
942 |
|
943 |
Vector3d ForceMatrixDecomposition::getIntergroupVector(int cg1, int cg2){ |
944 |
Vector3d d; |
945 |
|
946 |
#ifdef IS_MPI |
947 |
d = cgColData.position[cg2] - cgRowData.position[cg1]; |
948 |
#else |
949 |
d = snap_->cgData.position[cg2] - snap_->cgData.position[cg1]; |
950 |
#endif |
951 |
|
952 |
snap_->wrapVector(d); |
953 |
return d; |
954 |
} |
955 |
|
956 |
Vector3d ForceMatrixDecomposition::getGroupVelocityColumn(int cg2){ |
957 |
#ifdef IS_MPI |
958 |
return cgColData.velocity[cg2]; |
959 |
#else |
960 |
return snap_->cgData.velocity[cg2]; |
961 |
#endif |
962 |
} |
963 |
|
964 |
Vector3d ForceMatrixDecomposition::getAtomVelocityColumn(int atom2){ |
965 |
#ifdef IS_MPI |
966 |
return atomColData.velocity[atom2]; |
967 |
#else |
968 |
return snap_->atomData.velocity[atom2]; |
969 |
#endif |
970 |
} |
971 |
|
972 |
|
973 |
Vector3d ForceMatrixDecomposition::getAtomToGroupVectorRow(int atom1, int cg1){ |
974 |
|
975 |
Vector3d d; |
976 |
|
977 |
#ifdef IS_MPI |
978 |
d = cgRowData.position[cg1] - atomRowData.position[atom1]; |
979 |
#else |
980 |
d = snap_->cgData.position[cg1] - snap_->atomData.position[atom1]; |
981 |
#endif |
982 |
|
983 |
snap_->wrapVector(d); |
984 |
return d; |
985 |
} |
986 |
|
987 |
Vector3d ForceMatrixDecomposition::getAtomToGroupVectorColumn(int atom2, int cg2){ |
988 |
Vector3d d; |
989 |
|
990 |
#ifdef IS_MPI |
991 |
d = cgColData.position[cg2] - atomColData.position[atom2]; |
992 |
#else |
993 |
d = snap_->cgData.position[cg2] - snap_->atomData.position[atom2]; |
994 |
#endif |
995 |
|
996 |
snap_->wrapVector(d); |
997 |
return d; |
998 |
} |
999 |
|
1000 |
RealType ForceMatrixDecomposition::getMassFactorRow(int atom1) { |
1001 |
#ifdef IS_MPI |
1002 |
return massFactorsRow[atom1]; |
1003 |
#else |
1004 |
return massFactors[atom1]; |
1005 |
#endif |
1006 |
} |
1007 |
|
1008 |
RealType ForceMatrixDecomposition::getMassFactorColumn(int atom2) { |
1009 |
#ifdef IS_MPI |
1010 |
return massFactorsCol[atom2]; |
1011 |
#else |
1012 |
return massFactors[atom2]; |
1013 |
#endif |
1014 |
|
1015 |
} |
1016 |
|
1017 |
Vector3d ForceMatrixDecomposition::getInteratomicVector(int atom1, int atom2){ |
1018 |
Vector3d d; |
1019 |
|
1020 |
#ifdef IS_MPI |
1021 |
d = atomColData.position[atom2] - atomRowData.position[atom1]; |
1022 |
#else |
1023 |
d = snap_->atomData.position[atom2] - snap_->atomData.position[atom1]; |
1024 |
#endif |
1025 |
|
1026 |
snap_->wrapVector(d); |
1027 |
return d; |
1028 |
} |
1029 |
|
1030 |
vector<int> ForceMatrixDecomposition::getExcludesForAtom(int atom1) { |
1031 |
return excludesForAtom[atom1]; |
1032 |
} |
1033 |
|
1034 |
/** |
1035 |
* We need to exclude some overcounted interactions that result from |
1036 |
* the parallel decomposition. |
1037 |
*/ |
1038 |
bool ForceMatrixDecomposition::skipAtomPair(int atom1, int atom2, int cg1, int cg2) { |
1039 |
int unique_id_1, unique_id_2, group1, group2; |
1040 |
|
1041 |
#ifdef IS_MPI |
1042 |
// in MPI, we have to look up the unique IDs for each atom |
1043 |
unique_id_1 = AtomRowToGlobal[atom1]; |
1044 |
unique_id_2 = AtomColToGlobal[atom2]; |
1045 |
group1 = cgRowToGlobal[cg1]; |
1046 |
group2 = cgColToGlobal[cg2]; |
1047 |
#else |
1048 |
unique_id_1 = AtomLocalToGlobal[atom1]; |
1049 |
unique_id_2 = AtomLocalToGlobal[atom2]; |
1050 |
group1 = cgLocalToGlobal[cg1]; |
1051 |
group2 = cgLocalToGlobal[cg2]; |
1052 |
#endif |
1053 |
|
1054 |
if (unique_id_1 == unique_id_2) return true; |
1055 |
|
1056 |
#ifdef IS_MPI |
1057 |
// this prevents us from doing the pair on multiple processors |
1058 |
if (unique_id_1 < unique_id_2) { |
1059 |
if ((unique_id_1 + unique_id_2) % 2 == 0) return true; |
1060 |
} else { |
1061 |
if ((unique_id_1 + unique_id_2) % 2 == 1) return true; |
1062 |
} |
1063 |
#endif |
1064 |
|
1065 |
#ifndef IS_MPI |
1066 |
if (group1 == group2) { |
1067 |
if (unique_id_1 < unique_id_2) return true; |
1068 |
} |
1069 |
#endif |
1070 |
|
1071 |
return false; |
1072 |
} |
1073 |
|
1074 |
/** |
1075 |
* We need to handle the interactions for atoms who are involved in |
1076 |
* the same rigid body as well as some short range interactions |
1077 |
* (bonds, bends, torsions) differently from other interactions. |
1078 |
* We'll still visit the pairwise routines, but with a flag that |
1079 |
* tells those routines to exclude the pair from direct long range |
1080 |
* interactions. Some indirect interactions (notably reaction |
1081 |
* field) must still be handled for these pairs. |
1082 |
*/ |
1083 |
bool ForceMatrixDecomposition::excludeAtomPair(int atom1, int atom2) { |
1084 |
|
1085 |
// excludesForAtom was constructed to use row/column indices in the MPI |
1086 |
// version, and to use local IDs in the non-MPI version: |
1087 |
|
1088 |
for (vector<int>::iterator i = excludesForAtom[atom1].begin(); |
1089 |
i != excludesForAtom[atom1].end(); ++i) { |
1090 |
if ( (*i) == atom2 ) return true; |
1091 |
} |
1092 |
|
1093 |
return false; |
1094 |
} |
1095 |
|
1096 |
|
1097 |
void ForceMatrixDecomposition::addForceToAtomRow(int atom1, Vector3d fg){ |
1098 |
#ifdef IS_MPI |
1099 |
atomRowData.force[atom1] += fg; |
1100 |
#else |
1101 |
snap_->atomData.force[atom1] += fg; |
1102 |
#endif |
1103 |
} |
1104 |
|
1105 |
void ForceMatrixDecomposition::addForceToAtomColumn(int atom2, Vector3d fg){ |
1106 |
#ifdef IS_MPI |
1107 |
atomColData.force[atom2] += fg; |
1108 |
#else |
1109 |
snap_->atomData.force[atom2] += fg; |
1110 |
#endif |
1111 |
} |
1112 |
|
1113 |
// filling interaction blocks with pointers |
1114 |
void ForceMatrixDecomposition::fillInteractionData(InteractionData &idat, |
1115 |
int atom1, int atom2) { |
1116 |
|
1117 |
idat.excluded = excludeAtomPair(atom1, atom2); |
1118 |
|
1119 |
#ifdef IS_MPI |
1120 |
idat.atypes = make_pair( atypesRow[atom1], atypesCol[atom2]); |
1121 |
//idat.atypes = make_pair( ff_->getAtomType(identsRow[atom1]), |
1122 |
// ff_->getAtomType(identsCol[atom2]) ); |
1123 |
|
1124 |
if (storageLayout_ & DataStorage::dslAmat) { |
1125 |
idat.A1 = &(atomRowData.aMat[atom1]); |
1126 |
idat.A2 = &(atomColData.aMat[atom2]); |
1127 |
} |
1128 |
|
1129 |
if (storageLayout_ & DataStorage::dslElectroFrame) { |
1130 |
idat.eFrame1 = &(atomRowData.electroFrame[atom1]); |
1131 |
idat.eFrame2 = &(atomColData.electroFrame[atom2]); |
1132 |
} |
1133 |
|
1134 |
if (storageLayout_ & DataStorage::dslTorque) { |
1135 |
idat.t1 = &(atomRowData.torque[atom1]); |
1136 |
idat.t2 = &(atomColData.torque[atom2]); |
1137 |
} |
1138 |
|
1139 |
if (storageLayout_ & DataStorage::dslDensity) { |
1140 |
idat.rho1 = &(atomRowData.density[atom1]); |
1141 |
idat.rho2 = &(atomColData.density[atom2]); |
1142 |
} |
1143 |
|
1144 |
if (storageLayout_ & DataStorage::dslFunctional) { |
1145 |
idat.frho1 = &(atomRowData.functional[atom1]); |
1146 |
idat.frho2 = &(atomColData.functional[atom2]); |
1147 |
} |
1148 |
|
1149 |
if (storageLayout_ & DataStorage::dslFunctionalDerivative) { |
1150 |
idat.dfrho1 = &(atomRowData.functionalDerivative[atom1]); |
1151 |
idat.dfrho2 = &(atomColData.functionalDerivative[atom2]); |
1152 |
} |
1153 |
|
1154 |
if (storageLayout_ & DataStorage::dslParticlePot) { |
1155 |
idat.particlePot1 = &(atomRowData.particlePot[atom1]); |
1156 |
idat.particlePot2 = &(atomColData.particlePot[atom2]); |
1157 |
} |
1158 |
|
1159 |
if (storageLayout_ & DataStorage::dslSkippedCharge) { |
1160 |
idat.skippedCharge1 = &(atomRowData.skippedCharge[atom1]); |
1161 |
idat.skippedCharge2 = &(atomColData.skippedCharge[atom2]); |
1162 |
} |
1163 |
|
1164 |
if (storageLayout_ & DataStorage::dslFlucQPosition) { |
1165 |
idat.flucQ1 = &(atomRowData.flucQPos[atom1]); |
1166 |
idat.flucQ2 = &(atomColData.flucQPos[atom2]); |
1167 |
} |
1168 |
|
1169 |
#else |
1170 |
|
1171 |
idat.atypes = make_pair( atypesLocal[atom1], atypesLocal[atom2]); |
1172 |
|
1173 |
if (storageLayout_ & DataStorage::dslAmat) { |
1174 |
idat.A1 = &(snap_->atomData.aMat[atom1]); |
1175 |
idat.A2 = &(snap_->atomData.aMat[atom2]); |
1176 |
} |
1177 |
|
1178 |
if (storageLayout_ & DataStorage::dslElectroFrame) { |
1179 |
idat.eFrame1 = &(snap_->atomData.electroFrame[atom1]); |
1180 |
idat.eFrame2 = &(snap_->atomData.electroFrame[atom2]); |
1181 |
} |
1182 |
|
1183 |
if (storageLayout_ & DataStorage::dslTorque) { |
1184 |
idat.t1 = &(snap_->atomData.torque[atom1]); |
1185 |
idat.t2 = &(snap_->atomData.torque[atom2]); |
1186 |
} |
1187 |
|
1188 |
if (storageLayout_ & DataStorage::dslDensity) { |
1189 |
idat.rho1 = &(snap_->atomData.density[atom1]); |
1190 |
idat.rho2 = &(snap_->atomData.density[atom2]); |
1191 |
} |
1192 |
|
1193 |
if (storageLayout_ & DataStorage::dslFunctional) { |
1194 |
idat.frho1 = &(snap_->atomData.functional[atom1]); |
1195 |
idat.frho2 = &(snap_->atomData.functional[atom2]); |
1196 |
} |
1197 |
|
1198 |
if (storageLayout_ & DataStorage::dslFunctionalDerivative) { |
1199 |
idat.dfrho1 = &(snap_->atomData.functionalDerivative[atom1]); |
1200 |
idat.dfrho2 = &(snap_->atomData.functionalDerivative[atom2]); |
1201 |
} |
1202 |
|
1203 |
if (storageLayout_ & DataStorage::dslParticlePot) { |
1204 |
idat.particlePot1 = &(snap_->atomData.particlePot[atom1]); |
1205 |
idat.particlePot2 = &(snap_->atomData.particlePot[atom2]); |
1206 |
} |
1207 |
|
1208 |
if (storageLayout_ & DataStorage::dslSkippedCharge) { |
1209 |
idat.skippedCharge1 = &(snap_->atomData.skippedCharge[atom1]); |
1210 |
idat.skippedCharge2 = &(snap_->atomData.skippedCharge[atom2]); |
1211 |
} |
1212 |
|
1213 |
if (storageLayout_ & DataStorage::dslFlucQPosition) { |
1214 |
idat.flucQ1 = &(snap_->atomData.flucQPos[atom1]); |
1215 |
idat.flucQ2 = &(snap_->atomData.flucQPos[atom2]); |
1216 |
} |
1217 |
|
1218 |
#endif |
1219 |
} |
1220 |
|
1221 |
|
1222 |
void ForceMatrixDecomposition::unpackInteractionData(InteractionData &idat, int atom1, int atom2) { |
1223 |
#ifdef IS_MPI |
1224 |
pot_row[atom1] += RealType(0.5) * *(idat.pot); |
1225 |
pot_col[atom2] += RealType(0.5) * *(idat.pot); |
1226 |
expot_row[atom1] += RealType(0.5) * *(idat.excludedPot); |
1227 |
expot_col[atom2] += RealType(0.5) * *(idat.excludedPot); |
1228 |
|
1229 |
atomRowData.force[atom1] += *(idat.f1); |
1230 |
atomColData.force[atom2] -= *(idat.f1); |
1231 |
|
1232 |
if (storageLayout_ & DataStorage::dslFlucQForce) { |
1233 |
atomRowData.flucQFrc[atom1] -= *(idat.dVdFQ1); |
1234 |
atomColData.flucQFrc[atom2] -= *(idat.dVdFQ2); |
1235 |
} |
1236 |
|
1237 |
if (storageLayout_ & DataStorage::dslElectricField) { |
1238 |
atomRowData.electricField[atom1] += *(idat.eField1); |
1239 |
atomColData.electricField[atom2] += *(idat.eField2); |
1240 |
} |
1241 |
|
1242 |
#else |
1243 |
pairwisePot += *(idat.pot); |
1244 |
excludedPot += *(idat.excludedPot); |
1245 |
|
1246 |
snap_->atomData.force[atom1] += *(idat.f1); |
1247 |
snap_->atomData.force[atom2] -= *(idat.f1); |
1248 |
|
1249 |
if (idat.doParticlePot) { |
1250 |
// This is the pairwise contribution to the particle pot. The |
1251 |
// embedding contribution is added in each of the low level |
1252 |
// non-bonded routines. In parallel, this calculation is done |
1253 |
// in collectData, not in unpackInteractionData. |
1254 |
snap_->atomData.particlePot[atom1] += *(idat.vpair) * *(idat.sw); |
1255 |
snap_->atomData.particlePot[atom2] += *(idat.vpair) * *(idat.sw); |
1256 |
} |
1257 |
|
1258 |
if (storageLayout_ & DataStorage::dslFlucQForce) { |
1259 |
snap_->atomData.flucQFrc[atom1] -= *(idat.dVdFQ1); |
1260 |
snap_->atomData.flucQFrc[atom2] -= *(idat.dVdFQ2); |
1261 |
} |
1262 |
|
1263 |
if (storageLayout_ & DataStorage::dslElectricField) { |
1264 |
snap_->atomData.electricField[atom1] += *(idat.eField1); |
1265 |
snap_->atomData.electricField[atom2] += *(idat.eField2); |
1266 |
} |
1267 |
|
1268 |
#endif |
1269 |
|
1270 |
} |
1271 |
|
1272 |
/* |
1273 |
* buildNeighborList |
1274 |
* |
1275 |
* first element of pair is row-indexed CutoffGroup |
1276 |
* second element of pair is column-indexed CutoffGroup |
1277 |
*/ |
1278 |
vector<pair<int, int> > ForceMatrixDecomposition::buildNeighborList() { |
1279 |
|
1280 |
vector<pair<int, int> > neighborList; |
1281 |
groupCutoffs cuts; |
1282 |
bool doAllPairs = false; |
1283 |
|
1284 |
#ifdef IS_MPI |
1285 |
cellListRow_.clear(); |
1286 |
cellListCol_.clear(); |
1287 |
#else |
1288 |
cellList_.clear(); |
1289 |
#endif |
1290 |
|
1291 |
RealType rList_ = (largestRcut_ + skinThickness_); |
1292 |
RealType rl2 = rList_ * rList_; |
1293 |
Snapshot* snap_ = sman_->getCurrentSnapshot(); |
1294 |
Mat3x3d Hmat = snap_->getHmat(); |
1295 |
Vector3d Hx = Hmat.getColumn(0); |
1296 |
Vector3d Hy = Hmat.getColumn(1); |
1297 |
Vector3d Hz = Hmat.getColumn(2); |
1298 |
|
1299 |
nCells_.x() = (int) ( Hx.length() )/ rList_; |
1300 |
nCells_.y() = (int) ( Hy.length() )/ rList_; |
1301 |
nCells_.z() = (int) ( Hz.length() )/ rList_; |
1302 |
|
1303 |
// handle small boxes where the cell offsets can end up repeating cells |
1304 |
|
1305 |
if (nCells_.x() < 3) doAllPairs = true; |
1306 |
if (nCells_.y() < 3) doAllPairs = true; |
1307 |
if (nCells_.z() < 3) doAllPairs = true; |
1308 |
|
1309 |
Mat3x3d invHmat = snap_->getInvHmat(); |
1310 |
Vector3d rs, scaled, dr; |
1311 |
Vector3i whichCell; |
1312 |
int cellIndex; |
1313 |
int nCtot = nCells_.x() * nCells_.y() * nCells_.z(); |
1314 |
|
1315 |
#ifdef IS_MPI |
1316 |
cellListRow_.resize(nCtot); |
1317 |
cellListCol_.resize(nCtot); |
1318 |
#else |
1319 |
cellList_.resize(nCtot); |
1320 |
#endif |
1321 |
|
1322 |
if (!doAllPairs) { |
1323 |
#ifdef IS_MPI |
1324 |
|
1325 |
for (int i = 0; i < nGroupsInRow_; i++) { |
1326 |
rs = cgRowData.position[i]; |
1327 |
|
1328 |
// scaled positions relative to the box vectors |
1329 |
scaled = invHmat * rs; |
1330 |
|
1331 |
// wrap the vector back into the unit box by subtracting integer box |
1332 |
// numbers |
1333 |
for (int j = 0; j < 3; j++) { |
1334 |
scaled[j] -= roundMe(scaled[j]); |
1335 |
scaled[j] += 0.5; |
1336 |
} |
1337 |
|
1338 |
// find xyz-indices of cell that cutoffGroup is in. |
1339 |
whichCell.x() = nCells_.x() * scaled.x(); |
1340 |
whichCell.y() = nCells_.y() * scaled.y(); |
1341 |
whichCell.z() = nCells_.z() * scaled.z(); |
1342 |
|
1343 |
// find single index of this cell: |
1344 |
cellIndex = Vlinear(whichCell, nCells_); |
1345 |
|
1346 |
// add this cutoff group to the list of groups in this cell; |
1347 |
cellListRow_[cellIndex].push_back(i); |
1348 |
} |
1349 |
for (int i = 0; i < nGroupsInCol_; i++) { |
1350 |
rs = cgColData.position[i]; |
1351 |
|
1352 |
// scaled positions relative to the box vectors |
1353 |
scaled = invHmat * rs; |
1354 |
|
1355 |
// wrap the vector back into the unit box by subtracting integer box |
1356 |
// numbers |
1357 |
for (int j = 0; j < 3; j++) { |
1358 |
scaled[j] -= roundMe(scaled[j]); |
1359 |
scaled[j] += 0.5; |
1360 |
} |
1361 |
|
1362 |
// find xyz-indices of cell that cutoffGroup is in. |
1363 |
whichCell.x() = nCells_.x() * scaled.x(); |
1364 |
whichCell.y() = nCells_.y() * scaled.y(); |
1365 |
whichCell.z() = nCells_.z() * scaled.z(); |
1366 |
|
1367 |
// find single index of this cell: |
1368 |
cellIndex = Vlinear(whichCell, nCells_); |
1369 |
|
1370 |
// add this cutoff group to the list of groups in this cell; |
1371 |
cellListCol_[cellIndex].push_back(i); |
1372 |
} |
1373 |
|
1374 |
#else |
1375 |
for (int i = 0; i < nGroups_; i++) { |
1376 |
rs = snap_->cgData.position[i]; |
1377 |
|
1378 |
// scaled positions relative to the box vectors |
1379 |
scaled = invHmat * rs; |
1380 |
|
1381 |
// wrap the vector back into the unit box by subtracting integer box |
1382 |
// numbers |
1383 |
for (int j = 0; j < 3; j++) { |
1384 |
scaled[j] -= roundMe(scaled[j]); |
1385 |
scaled[j] += 0.5; |
1386 |
} |
1387 |
|
1388 |
// find xyz-indices of cell that cutoffGroup is in. |
1389 |
whichCell.x() = nCells_.x() * scaled.x(); |
1390 |
whichCell.y() = nCells_.y() * scaled.y(); |
1391 |
whichCell.z() = nCells_.z() * scaled.z(); |
1392 |
|
1393 |
// find single index of this cell: |
1394 |
cellIndex = Vlinear(whichCell, nCells_); |
1395 |
|
1396 |
// add this cutoff group to the list of groups in this cell; |
1397 |
cellList_[cellIndex].push_back(i); |
1398 |
} |
1399 |
|
1400 |
#endif |
1401 |
|
1402 |
for (int m1z = 0; m1z < nCells_.z(); m1z++) { |
1403 |
for (int m1y = 0; m1y < nCells_.y(); m1y++) { |
1404 |
for (int m1x = 0; m1x < nCells_.x(); m1x++) { |
1405 |
Vector3i m1v(m1x, m1y, m1z); |
1406 |
int m1 = Vlinear(m1v, nCells_); |
1407 |
|
1408 |
for (vector<Vector3i>::iterator os = cellOffsets_.begin(); |
1409 |
os != cellOffsets_.end(); ++os) { |
1410 |
|
1411 |
Vector3i m2v = m1v + (*os); |
1412 |
|
1413 |
|
1414 |
if (m2v.x() >= nCells_.x()) { |
1415 |
m2v.x() = 0; |
1416 |
} else if (m2v.x() < 0) { |
1417 |
m2v.x() = nCells_.x() - 1; |
1418 |
} |
1419 |
|
1420 |
if (m2v.y() >= nCells_.y()) { |
1421 |
m2v.y() = 0; |
1422 |
} else if (m2v.y() < 0) { |
1423 |
m2v.y() = nCells_.y() - 1; |
1424 |
} |
1425 |
|
1426 |
if (m2v.z() >= nCells_.z()) { |
1427 |
m2v.z() = 0; |
1428 |
} else if (m2v.z() < 0) { |
1429 |
m2v.z() = nCells_.z() - 1; |
1430 |
} |
1431 |
|
1432 |
int m2 = Vlinear (m2v, nCells_); |
1433 |
|
1434 |
#ifdef IS_MPI |
1435 |
for (vector<int>::iterator j1 = cellListRow_[m1].begin(); |
1436 |
j1 != cellListRow_[m1].end(); ++j1) { |
1437 |
for (vector<int>::iterator j2 = cellListCol_[m2].begin(); |
1438 |
j2 != cellListCol_[m2].end(); ++j2) { |
1439 |
|
1440 |
// In parallel, we need to visit *all* pairs of row |
1441 |
// & column indicies and will divide labor in the |
1442 |
// force evaluation later. |
1443 |
dr = cgColData.position[(*j2)] - cgRowData.position[(*j1)]; |
1444 |
snap_->wrapVector(dr); |
1445 |
cuts = getGroupCutoffs( (*j1), (*j2) ); |
1446 |
if (dr.lengthSquare() < cuts.third) { |
1447 |
neighborList.push_back(make_pair((*j1), (*j2))); |
1448 |
} |
1449 |
} |
1450 |
} |
1451 |
#else |
1452 |
for (vector<int>::iterator j1 = cellList_[m1].begin(); |
1453 |
j1 != cellList_[m1].end(); ++j1) { |
1454 |
for (vector<int>::iterator j2 = cellList_[m2].begin(); |
1455 |
j2 != cellList_[m2].end(); ++j2) { |
1456 |
|
1457 |
// Always do this if we're in different cells or if |
1458 |
// we're in the same cell and the global index of |
1459 |
// the j2 cutoff group is greater than or equal to |
1460 |
// the j1 cutoff group. Note that Rappaport's code |
1461 |
// has a "less than" conditional here, but that |
1462 |
// deals with atom-by-atom computation. OpenMD |
1463 |
// allows atoms within a single cutoff group to |
1464 |
// interact with each other. |
1465 |
|
1466 |
|
1467 |
|
1468 |
if (m2 != m1 || (*j2) >= (*j1) ) { |
1469 |
|
1470 |
dr = snap_->cgData.position[(*j2)] - snap_->cgData.position[(*j1)]; |
1471 |
snap_->wrapVector(dr); |
1472 |
cuts = getGroupCutoffs( (*j1), (*j2) ); |
1473 |
if (dr.lengthSquare() < cuts.third) { |
1474 |
neighborList.push_back(make_pair((*j1), (*j2))); |
1475 |
} |
1476 |
} |
1477 |
} |
1478 |
} |
1479 |
#endif |
1480 |
} |
1481 |
} |
1482 |
} |
1483 |
} |
1484 |
} else { |
1485 |
// branch to do all cutoff group pairs |
1486 |
#ifdef IS_MPI |
1487 |
for (int j1 = 0; j1 < nGroupsInRow_; j1++) { |
1488 |
for (int j2 = 0; j2 < nGroupsInCol_; j2++) { |
1489 |
dr = cgColData.position[j2] - cgRowData.position[j1]; |
1490 |
snap_->wrapVector(dr); |
1491 |
cuts = getGroupCutoffs( j1, j2 ); |
1492 |
if (dr.lengthSquare() < cuts.third) { |
1493 |
neighborList.push_back(make_pair(j1, j2)); |
1494 |
} |
1495 |
} |
1496 |
} |
1497 |
#else |
1498 |
// include all groups here. |
1499 |
for (int j1 = 0; j1 < nGroups_; j1++) { |
1500 |
// include self group interactions j2 == j1 |
1501 |
for (int j2 = j1; j2 < nGroups_; j2++) { |
1502 |
dr = snap_->cgData.position[j2] - snap_->cgData.position[j1]; |
1503 |
snap_->wrapVector(dr); |
1504 |
cuts = getGroupCutoffs( j1, j2 ); |
1505 |
if (dr.lengthSquare() < cuts.third) { |
1506 |
neighborList.push_back(make_pair(j1, j2)); |
1507 |
} |
1508 |
} |
1509 |
} |
1510 |
#endif |
1511 |
} |
1512 |
|
1513 |
// save the local cutoff group positions for the check that is |
1514 |
// done on each loop: |
1515 |
saved_CG_positions_.clear(); |
1516 |
for (int i = 0; i < nGroups_; i++) |
1517 |
saved_CG_positions_.push_back(snap_->cgData.position[i]); |
1518 |
|
1519 |
return neighborList; |
1520 |
} |
1521 |
} //end namespace OpenMD |