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40 * \brief This file defines integrators for energy minimization
42 * \author Berk Hess <hess@kth.se>
43 * \author Erik Lindahl <erik@kth.se>
44 * \ingroup module_mdrun
58 #include "gromacs/commandline/filenm.h"
59 #include "gromacs/domdec/collect.h"
60 #include "gromacs/domdec/dlbtiming.h"
61 #include "gromacs/domdec/domdec.h"
62 #include "gromacs/domdec/domdec_struct.h"
63 #include "gromacs/domdec/mdsetup.h"
64 #include "gromacs/domdec/partition.h"
65 #include "gromacs/ewald/pme_pp.h"
66 #include "gromacs/fileio/confio.h"
67 #include "gromacs/fileio/mtxio.h"
68 #include "gromacs/gmxlib/network.h"
69 #include "gromacs/gmxlib/nrnb.h"
70 #include "gromacs/imd/imd.h"
71 #include "gromacs/linearalgebra/sparsematrix.h"
72 #include "gromacs/listed_forces/listed_forces.h"
73 #include "gromacs/math/functions.h"
74 #include "gromacs/math/vec.h"
75 #include "gromacs/mdlib/constr.h"
76 #include "gromacs/mdlib/coupling.h"
77 #include "gromacs/mdlib/dispersioncorrection.h"
78 #include "gromacs/mdlib/ebin.h"
79 #include "gromacs/mdlib/enerdata_utils.h"
80 #include "gromacs/mdlib/energyoutput.h"
81 #include "gromacs/mdlib/force.h"
82 #include "gromacs/mdlib/force_flags.h"
83 #include "gromacs/mdlib/forcerec.h"
84 #include "gromacs/mdlib/gmx_omp_nthreads.h"
85 #include "gromacs/mdlib/md_support.h"
86 #include "gromacs/mdlib/mdatoms.h"
87 #include "gromacs/mdlib/stat.h"
88 #include "gromacs/mdlib/tgroup.h"
89 #include "gromacs/mdlib/trajectory_writing.h"
90 #include "gromacs/mdlib/update.h"
91 #include "gromacs/mdlib/vsite.h"
92 #include "gromacs/mdrunutility/handlerestart.h"
93 #include "gromacs/mdrunutility/printtime.h"
94 #include "gromacs/mdtypes/checkpointdata.h"
95 #include "gromacs/mdtypes/commrec.h"
96 #include "gromacs/mdtypes/forcebuffers.h"
97 #include "gromacs/mdtypes/forcerec.h"
98 #include "gromacs/mdtypes/inputrec.h"
99 #include "gromacs/mdtypes/interaction_const.h"
100 #include "gromacs/mdtypes/md_enums.h"
101 #include "gromacs/mdtypes/mdatom.h"
102 #include "gromacs/mdtypes/mdrunoptions.h"
103 #include "gromacs/mdtypes/observablesreducer.h"
104 #include "gromacs/mdtypes/state.h"
105 #include "gromacs/pbcutil/pbc.h"
106 #include "gromacs/timing/wallcycle.h"
107 #include "gromacs/timing/walltime_accounting.h"
108 #include "gromacs/topology/mtop_util.h"
109 #include "gromacs/topology/topology.h"
110 #include "gromacs/utility/cstringutil.h"
111 #include "gromacs/utility/exceptions.h"
112 #include "gromacs/utility/fatalerror.h"
113 #include "gromacs/utility/logger.h"
114 #include "gromacs/utility/smalloc.h"
116 #include "legacysimulator.h"
120 using gmx::MdrunScheduleWorkload;
122 using gmx::VirtualSitesHandler;
124 //! Utility structure for manipulating states during EM
125 typedef struct em_state
127 //! Copy of the global state
133 //! Norm of the force
141 //! Print the EM starting conditions
142 static void print_em_start(FILE* fplog,
144 gmx_walltime_accounting_t walltime_accounting,
145 gmx_wallcycle* wcycle,
148 walltime_accounting_start_time(walltime_accounting);
149 wallcycle_start(wcycle, WallCycleCounter::Run);
150 print_start(fplog, cr, walltime_accounting, name);
153 //! Stop counting time for EM
154 static void em_time_end(gmx_walltime_accounting_t walltime_accounting, gmx_wallcycle* wcycle)
156 wallcycle_stop(wcycle, WallCycleCounter::Run);
158 walltime_accounting_end_time(walltime_accounting);
161 //! Printing a log file and console header
162 static void sp_header(FILE* out, const char* minimizer, real ftol, int nsteps)
165 fprintf(out, "%s:\n", minimizer);
166 fprintf(out, " Tolerance (Fmax) = %12.5e\n", ftol);
167 fprintf(out, " Number of steps = %12d\n", nsteps);
170 //! Print warning message
171 static void warn_step(FILE* fp, real ftol, real fmax, gmx_bool bLastStep, gmx_bool bConstrain)
173 constexpr bool realIsDouble = GMX_DOUBLE;
176 if (!std::isfinite(fmax))
179 "\nEnergy minimization has stopped because the force "
180 "on at least one atom is not finite. This usually means "
181 "atoms are overlapping. Modify the input coordinates to "
182 "remove atom overlap or use soft-core potentials with "
183 "the free energy code to avoid infinite forces.\n%s",
184 !realIsDouble ? "You could also be lucky that switching to double precision "
185 "is sufficient to obtain finite forces.\n"
191 "\nEnergy minimization reached the maximum number "
192 "of steps before the forces reached the requested "
193 "precision Fmax < %g.\n",
199 "\nEnergy minimization has stopped, but the forces have "
200 "not converged to the requested precision Fmax < %g (which "
201 "may not be possible for your system). It stopped "
202 "because the algorithm tried to make a new step whose size "
203 "was too small, or there was no change in the energy since "
204 "last step. Either way, we regard the minimization as "
205 "converged to within the available machine precision, "
206 "given your starting configuration and EM parameters.\n%s%s",
208 !realIsDouble ? "\nDouble precision normally gives you higher accuracy, but "
209 "this is often not needed for preparing to run molecular "
212 bConstrain ? "You might need to increase your constraint accuracy, or turn\n"
213 "off constraints altogether (set constraints = none in mdp file)\n"
217 fputs(wrap_lines(buffer, 78, 0, FALSE), stderr);
218 fputs(wrap_lines(buffer, 78, 0, FALSE), fp);
221 //! Print message about convergence of the EM
222 static void print_converged(FILE* fp,
228 const em_state_t* ems,
231 char buf[STEPSTRSIZE];
235 fprintf(fp, "\n%s converged to Fmax < %g in %s steps\n", alg, ftol, gmx_step_str(count, buf));
237 else if (count < nsteps)
240 "\n%s converged to machine precision in %s steps,\n"
241 "but did not reach the requested Fmax < %g.\n",
243 gmx_step_str(count, buf),
248 fprintf(fp, "\n%s did not converge to Fmax < %g in %s steps.\n", alg, ftol, gmx_step_str(count, buf));
252 fprintf(fp, "Potential Energy = %21.14e\n", ems->epot);
253 fprintf(fp, "Maximum force = %21.14e on atom %d\n", ems->fmax, ems->a_fmax + 1);
254 fprintf(fp, "Norm of force = %21.14e\n", ems->fnorm / sqrtNumAtoms);
256 fprintf(fp, "Potential Energy = %14.7e\n", ems->epot);
257 fprintf(fp, "Maximum force = %14.7e on atom %d\n", ems->fmax, ems->a_fmax + 1);
258 fprintf(fp, "Norm of force = %14.7e\n", ems->fnorm / sqrtNumAtoms);
262 //! Compute the norm and max of the force array in parallel
263 static void get_f_norm_max(const t_commrec* cr,
264 const t_grpopts* opts,
266 gmx::ArrayRef<const gmx::RVec> f,
273 int la_max, a_max, start, end, i, m, gf;
275 /* This routine finds the largest force and returns it.
276 * On parallel machines the global max is taken.
282 end = mdatoms->homenr;
283 if (mdatoms->cFREEZE)
285 for (i = start; i < end; i++)
287 gf = mdatoms->cFREEZE[i];
289 for (m = 0; m < DIM; m++)
291 if (!opts->nFreeze[gf][m])
293 fam += gmx::square(f[i][m]);
306 for (i = start; i < end; i++)
318 if (la_max >= 0 && DOMAINDECOMP(cr))
320 a_max = cr->dd->globalAtomIndices[la_max];
328 snew(sum, 2 * cr->nnodes + 1);
329 sum[2 * cr->nodeid] = fmax2;
330 sum[2 * cr->nodeid + 1] = a_max;
331 sum[2 * cr->nnodes] = fnorm2;
332 gmx_sumd(2 * cr->nnodes + 1, sum, cr);
333 fnorm2 = sum[2 * cr->nnodes];
334 /* Determine the global maximum */
335 for (i = 0; i < cr->nnodes; i++)
337 if (sum[2 * i] > fmax2)
340 a_max = gmx::roundToInt(sum[2 * i + 1]);
348 *fnorm = sqrt(fnorm2);
360 //! Compute the norm of the force
361 static void get_state_f_norm_max(const t_commrec* cr, const t_grpopts* opts, t_mdatoms* mdatoms, em_state_t* ems)
363 get_f_norm_max(cr, opts, mdatoms, ems->f.view().force(), &ems->fnorm, &ems->fmax, &ems->a_fmax);
366 //! Initialize the energy minimization
367 static void init_em(FILE* fplog,
368 const gmx::MDLogger& mdlog,
371 const t_inputrec* ir,
372 gmx::ImdSession* imdSession,
374 t_state* state_global,
375 const gmx_mtop_t& top_global,
380 gmx::MDAtoms* mdAtoms,
381 gmx_global_stat_t* gstat,
382 VirtualSitesHandler* vsite,
383 gmx::Constraints* constr,
384 gmx_shellfc_t** shellfc)
390 fprintf(fplog, "Initiating %s\n", title);
395 state_global->ngtc = 0;
397 int* fep_state = MASTER(cr) ? &state_global->fep_state : nullptr;
398 gmx::ArrayRef<real> lambda = MASTER(cr) ? state_global->lambda : gmx::ArrayRef<real>();
399 initialize_lambdas(fplog,
403 ir->simtempvals->temperatures,
404 gmx::arrayRefFromArray(ir->opts.ref_t, ir->opts.ngtc),
409 if (ir->eI == IntegrationAlgorithm::NM)
411 GMX_ASSERT(shellfc != nullptr, "With NM we always support shells");
413 *shellfc = init_shell_flexcon(stdout,
415 constr ? constr->numFlexibleConstraints() : 0,
418 thisRankHasDuty(cr, DUTY_PME));
422 GMX_ASSERT(EI_ENERGY_MINIMIZATION(ir->eI),
423 "This else currently only handles energy minimizers, consider if your algorithm "
424 "needs shell/flexible-constraint support");
426 /* With energy minimization, shells and flexible constraints are
427 * automatically minimized when treated like normal DOFS.
429 if (shellfc != nullptr)
435 if (DOMAINDECOMP(cr))
437 dd_init_local_state(*cr->dd, state_global, &ems->s);
439 /* Distribute the charge groups over the nodes from the master node */
440 dd_partition_system(fplog,
461 dd_store_state(*cr->dd, &ems->s);
465 state_change_natoms(state_global, state_global->natoms);
466 /* Just copy the state */
467 ems->s = *state_global;
468 state_change_natoms(&ems->s, ems->s.natoms);
470 mdAlgorithmsSetupAtomData(
471 cr, *ir, top_global, top, fr, &ems->f, mdAtoms, constr, vsite, shellfc ? *shellfc : nullptr);
474 update_mdatoms(mdAtoms->mdatoms(), ems->s.lambda[FreeEnergyPerturbationCouplingType::Mass]);
478 // TODO how should this cross-module support dependency be managed?
479 if (ir->eConstrAlg == ConstraintAlgorithm::Shake && gmx_mtop_ftype_count(top_global, F_CONSTR) > 0)
482 "Can not do energy minimization with %s, use %s\n",
483 enumValueToString(ConstraintAlgorithm::Shake),
484 enumValueToString(ConstraintAlgorithm::Lincs));
487 if (!ir->bContinuation)
489 /* Constrain the starting coordinates */
490 bool needsLogging = true;
491 bool computeEnergy = true;
492 bool computeVirial = false;
494 constr->apply(needsLogging,
499 ems->s.x.arrayRefWithPadding(),
500 ems->s.x.arrayRefWithPadding(),
503 ems->s.lambda[FreeEnergyPerturbationCouplingType::Fep],
505 gmx::ArrayRefWithPadding<RVec>(),
508 gmx::ConstraintVariable::Positions);
514 *gstat = global_stat_init(ir);
521 calc_shifts(ems->s.box, fr->shift_vec);
524 //! Finalize the minimization
525 static void finish_em(const t_commrec* cr,
527 gmx_walltime_accounting_t walltime_accounting,
528 gmx_wallcycle* wcycle)
530 if (!thisRankHasDuty(cr, DUTY_PME))
532 /* Tell the PME only node to finish */
533 gmx_pme_send_finish(cr);
538 em_time_end(walltime_accounting, wcycle);
541 //! Swap two different EM states during minimization
542 static void swap_em_state(em_state_t** ems1, em_state_t** ems2)
551 //! Save the EM trajectory
552 static void write_em_traj(FILE* fplog,
558 const gmx_mtop_t& top_global,
559 const t_inputrec* ir,
562 t_state* state_global,
563 ObservablesHistory* observablesHistory)
569 mdof_flags |= MDOF_X;
573 mdof_flags |= MDOF_F;
576 /* If we want IMD output, set appropriate MDOF flag */
579 mdof_flags |= MDOF_IMD;
582 gmx::WriteCheckpointDataHolder checkpointDataHolder;
583 mdoutf_write_to_trajectory_files(fplog,
589 static_cast<double>(step),
593 state->f.view().force(),
594 &checkpointDataHolder);
596 if (confout != nullptr)
598 if (DOMAINDECOMP(cr))
600 /* If bX=true, x was collected to state_global in the call above */
603 auto globalXRef = MASTER(cr) ? state_global->x : gmx::ArrayRef<gmx::RVec>();
605 cr->dd, state->s.ddp_count, state->s.ddp_count_cg_gl, state->s.cg_gl, state->s.x, globalXRef);
610 /* Copy the local state pointer */
611 state_global = &state->s;
616 if (ir->pbcType != PbcType::No && !ir->bPeriodicMols && DOMAINDECOMP(cr))
618 /* Make molecules whole only for confout writing */
619 do_pbc_mtop(ir->pbcType, state->s.box, &top_global, state_global->x.rvec_array());
622 write_sto_conf_mtop(confout,
625 state_global->x.rvec_array(),
633 //! \brief Do one minimization step
635 // \returns true when the step succeeded, false when a constraint error occurred
636 static bool do_em_step(const t_commrec* cr,
637 const t_inputrec* ir,
641 gmx::ArrayRefWithPadding<const gmx::RVec> force,
643 gmx::Constraints* constr,
650 int nthreads gmx_unused;
652 bool validStep = true;
657 if (DOMAINDECOMP(cr) && s1->ddp_count != cr->dd->ddp_count)
659 gmx_incons("state mismatch in do_em_step");
662 s2->flags = s1->flags;
664 if (s2->natoms != s1->natoms)
666 state_change_natoms(s2, s1->natoms);
667 ems2->f.resize(s2->natoms);
669 if (DOMAINDECOMP(cr) && s2->cg_gl.size() != s1->cg_gl.size())
671 s2->cg_gl.resize(s1->cg_gl.size());
674 copy_mat(s1->box, s2->box);
675 /* Copy free energy state */
676 s2->lambda = s1->lambda;
677 copy_mat(s1->box, s2->box);
682 nthreads = gmx_omp_nthreads_get(ModuleMultiThread::Update);
683 #pragma omp parallel num_threads(nthreads)
685 const rvec* x1 = s1->x.rvec_array();
686 rvec* x2 = s2->x.rvec_array();
687 const rvec* f = as_rvec_array(force.unpaddedArrayRef().data());
690 #pragma omp for schedule(static) nowait
691 for (int i = start; i < end; i++)
699 for (int m = 0; m < DIM; m++)
701 if (ir->opts.nFreeze[gf][m])
707 x2[i][m] = x1[i][m] + a * f[i][m];
711 GMX_CATCH_ALL_AND_EXIT_WITH_FATAL_ERROR
714 if (s2->flags & enumValueToBitMask(StateEntry::Cgp))
716 /* Copy the CG p vector */
717 const rvec* p1 = s1->cg_p.rvec_array();
718 rvec* p2 = s2->cg_p.rvec_array();
719 #pragma omp for schedule(static) nowait
720 for (int i = start; i < end; i++)
722 // Trivial OpenMP block that does not throw
723 copy_rvec(p1[i], p2[i]);
727 if (DOMAINDECOMP(cr))
729 /* OpenMP does not supported unsigned loop variables */
730 #pragma omp for schedule(static) nowait
731 for (gmx::index i = 0; i < gmx::ssize(s2->cg_gl); i++)
733 s2->cg_gl[i] = s1->cg_gl[i];
738 if (DOMAINDECOMP(cr))
740 s2->ddp_count = s1->ddp_count;
741 s2->ddp_count_cg_gl = s1->ddp_count_cg_gl;
747 validStep = constr->apply(TRUE,
752 s1->x.arrayRefWithPadding(),
753 s2->x.arrayRefWithPadding(),
756 s2->lambda[FreeEnergyPerturbationCouplingType::Bonded],
758 gmx::ArrayRefWithPadding<RVec>(),
761 gmx::ConstraintVariable::Positions);
765 /* This global reduction will affect performance at high
766 * parallelization, but we can not really avoid it.
767 * But usually EM is not run at high parallelization.
769 int reductionBuffer = static_cast<int>(!validStep);
770 gmx_sumi(1, &reductionBuffer, cr);
771 validStep = (reductionBuffer == 0);
774 // We should move this check to the different minimizers
775 if (!validStep && ir->eI != IntegrationAlgorithm::Steep)
778 "The coordinates could not be constrained. Minimizer '%s' can not handle "
779 "constraint failures, use minimizer '%s' before using '%s'.",
780 enumValueToString(ir->eI),
781 enumValueToString(IntegrationAlgorithm::Steep),
782 enumValueToString(ir->eI));
789 //! Prepare EM for using domain decomposition parallellization
790 static void em_dd_partition_system(FILE* fplog,
791 const gmx::MDLogger& mdlog,
794 const gmx_mtop_t& top_global,
795 const t_inputrec* ir,
796 gmx::ImdSession* imdSession,
800 gmx::MDAtoms* mdAtoms,
802 VirtualSitesHandler* vsite,
803 gmx::Constraints* constr,
805 gmx_wallcycle* wcycle)
807 /* Repartition the domain decomposition */
808 dd_partition_system(fplog,
829 dd_store_state(*cr->dd, &ems->s);
835 //! Copy coordinates, OpenMP parallelized, from \p refCoords to coords
836 void setCoordinates(std::vector<RVec>* coords, ArrayRef<const RVec> refCoords)
838 coords->resize(refCoords.size());
840 const int gmx_unused nthreads = gmx_omp_nthreads_get(ModuleMultiThread::Update);
841 #pragma omp parallel for num_threads(nthreads) schedule(static)
842 for (int i = 0; i < ssize(refCoords); i++)
844 (*coords)[i] = refCoords[i];
848 //! Returns the maximum difference an atom moved between two coordinate sets, over all ranks
849 real maxCoordinateDifference(ArrayRef<const RVec> coords1, ArrayRef<const RVec> coords2, MPI_Comm mpiCommMyGroup)
851 GMX_RELEASE_ASSERT(coords1.size() == coords2.size(), "Coordinate counts should match");
853 real maxDiffSquared = 0;
855 const int gmx_unused nthreads = gmx_omp_nthreads_get(ModuleMultiThread::Update);
856 #pragma omp parallel for reduction(max : maxDiffSquared) num_threads(nthreads) schedule(static)
857 for (int i = 0; i < ssize(coords1); i++)
859 maxDiffSquared = std::max(maxDiffSquared, gmx::norm2(coords1[i] - coords2[i]));
864 if (mpiCommMyGroup != MPI_COMM_NULL)
866 MPI_Comm_size(mpiCommMyGroup, &numRanks);
870 real maxDiffSquaredReduced;
872 &maxDiffSquared, &maxDiffSquaredReduced, 1, GMX_DOUBLE ? MPI_DOUBLE : MPI_FLOAT, MPI_MAX, mpiCommMyGroup);
873 maxDiffSquared = maxDiffSquaredReduced;
876 GMX_UNUSED_VALUE(mpiCommMyGroup);
879 return std::sqrt(maxDiffSquared);
882 /*! \brief Class to handle the work of setting and doing an energy evaluation.
884 * This class is a mere aggregate of parameters to pass to evaluate an
885 * energy, so that future changes to names and types of them consume
886 * less time when refactoring other code.
888 * Aggregate initialization is used, for which the chief risk is that
889 * if a member is added at the end and not all initializer lists are
890 * updated, then the member will be value initialized, which will
891 * typically mean initialization to zero.
893 * Use a braced initializer list to construct one of these. */
894 class EnergyEvaluator
897 /*! \brief Evaluates an energy on the state in \c ems.
899 * \todo In practice, the same objects mu_tot, vir, and pres
900 * are always passed to this function, so we would rather have
901 * them as data members. However, their C-array types are
902 * unsuited for aggregate initialization. When the types
903 * improve, the call signature of this method can be reduced.
905 void run(em_state_t* ems, rvec mu_tot, tensor vir, tensor pres, int64_t count, gmx_bool bFirst, int64_t step);
906 //! Handles logging (deprecated).
909 const gmx::MDLogger& mdlog;
910 //! Handles communication.
912 //! Coordinates multi-simulations.
913 const gmx_multisim_t* ms;
914 //! Holds the simulation topology.
915 const gmx_mtop_t& top_global;
916 //! Holds the domain topology.
918 //! User input options.
919 const t_inputrec* inputrec;
920 //! The Interactive Molecular Dynamics session.
921 gmx::ImdSession* imdSession;
922 //! The pull work object.
924 //! Manages flop accounting.
926 //! Manages wall cycle accounting.
927 gmx_wallcycle* wcycle;
928 //! Legacy coordinator of global reduction.
929 gmx_global_stat_t gstat;
930 //! Coordinates reduction for observables
931 gmx::ObservablesReducer* observablesReducer;
932 //! Handles virtual sites.
933 VirtualSitesHandler* vsite;
934 //! Handles constraints.
935 gmx::Constraints* constr;
936 //! Per-atom data for this domain.
937 gmx::MDAtoms* mdAtoms;
938 //! Handles how to calculate the forces.
940 //! Schedule of force-calculation work each step for this task.
941 MdrunScheduleWorkload* runScheduleWork;
942 //! Stores the computed energies.
943 gmx_enerdata_t* enerd;
944 //! The DD partitioning count at which the pair list was generated
945 int ddpCountPairSearch;
946 //! The local coordinates that were used for pair searching, stored for computing displacements
947 std::vector<RVec> pairSearchCoordinates;
950 void EnergyEvaluator::run(em_state_t* ems, rvec mu_tot, tensor vir, tensor pres, int64_t count, gmx_bool bFirst, int64_t step)
954 tensor force_vir, shake_vir, ekin;
958 /* Set the time to the initial time, the time does not change during EM */
959 t = inputrec->init_t;
963 vsite->construct(ems->s.x, {}, ems->s.box, gmx::VSiteOperation::Positions);
966 // Compute the buffer size of the pair list
967 const real bufferSize = inputrec->rlist - std::max(inputrec->rcoulomb, inputrec->rvdw);
969 if (bFirst || bufferSize <= 0 || (DOMAINDECOMP(cr) && ems->s.ddp_count != ddpCountPairSearch))
971 /* This is the first state or an old state used before the last ns */
976 // We need to generate a new pairlist when one atom moved more than half the buffer size
977 ArrayRef<const RVec> localCoordinates =
978 ArrayRef<const RVec>(ems->s.x).subArray(0, mdAtoms->mdatoms()->homenr);
979 bNS = 2 * maxCoordinateDifference(pairSearchCoordinates, localCoordinates, cr->mpi_comm_mygroup)
983 if (DOMAINDECOMP(cr) && bNS)
985 /* Repartition the domain decomposition */
986 em_dd_partition_system(
987 fplog, mdlog, count, cr, top_global, inputrec, imdSession, pull_work, ems, top, mdAtoms, fr, vsite, constr, nrnb, wcycle);
988 ddpCountPairSearch = cr->dd->ddp_count;
991 /* Store the local coordinates that will be used in the pair search, after we re-partitioned */
992 if (bufferSize > 0 && bNS)
994 ArrayRef<const RVec> localCoordinates =
995 constArrayRefFromArray(ems->s.x.data(), mdAtoms->mdatoms()->homenr);
996 setCoordinates(&pairSearchCoordinates, localCoordinates);
999 /* Calc force & energy on new trial position */
1000 /* do_force always puts the charge groups in the box and shifts again
1001 * We do not unshift, so molecules are always whole in congrad.c
1016 ems->s.x.arrayRefWithPadding(),
1029 GMX_FORCE_STATECHANGED | GMX_FORCE_ALLFORCES | GMX_FORCE_VIRIAL | GMX_FORCE_ENERGY
1030 | (bNS ? GMX_FORCE_NS : 0),
1031 DDBalanceRegionHandler(cr));
1033 /* Clear the unused shake virial and pressure */
1034 clear_mat(shake_vir);
1037 /* Communicate stuff when parallel */
1038 if (PAR(cr) && inputrec->eI != IntegrationAlgorithm::NM)
1040 wallcycle_start(wcycle, WallCycleCounter::MoveE);
1049 gmx::ArrayRef<real>{},
1051 std::vector<real>(1, terminate),
1053 CGLO_ENERGY | CGLO_PRESSURE | CGLO_CONSTRAINT,
1055 observablesReducer);
1057 wallcycle_stop(wcycle, WallCycleCounter::MoveE);
1060 if (fr->dispersionCorrection)
1062 /* Calculate long range corrections to pressure and energy */
1063 const DispersionCorrection::Correction correction = fr->dispersionCorrection->calculate(
1064 ems->s.box, ems->s.lambda[FreeEnergyPerturbationCouplingType::Vdw]);
1066 enerd->term[F_DISPCORR] = correction.energy;
1067 enerd->term[F_EPOT] += correction.energy;
1068 enerd->term[F_PRES] += correction.pressure;
1069 enerd->term[F_DVDL] += correction.dvdl;
1073 enerd->term[F_DISPCORR] = 0;
1076 ems->epot = enerd->term[F_EPOT];
1080 /* Project out the constraint components of the force */
1081 bool needsLogging = false;
1082 bool computeEnergy = false;
1083 bool computeVirial = true;
1085 auto f = ems->f.view().forceWithPadding();
1086 constr->apply(needsLogging,
1091 ems->s.x.arrayRefWithPadding(),
1093 f.unpaddedArrayRef(),
1095 ems->s.lambda[FreeEnergyPerturbationCouplingType::Bonded],
1097 gmx::ArrayRefWithPadding<RVec>(),
1100 gmx::ConstraintVariable::ForceDispl);
1101 enerd->term[F_DVDL_CONSTR] += dvdl_constr;
1102 m_add(force_vir, shake_vir, vir);
1106 copy_mat(force_vir, vir);
1110 enerd->term[F_PRES] = calc_pres(fr->pbcType, inputrec->nwall, ems->s.box, ekin, vir, pres);
1112 if (inputrec->efep != FreeEnergyPerturbationType::No)
1114 accumulateKineticLambdaComponents(enerd, ems->s.lambda, *inputrec->fepvals);
1117 if (EI_ENERGY_MINIMIZATION(inputrec->eI))
1119 get_state_f_norm_max(cr, &(inputrec->opts), mdAtoms->mdatoms(), ems);
1125 //! Parallel utility summing energies and forces
1126 static double reorder_partsum(const t_commrec* cr,
1127 const t_grpopts* opts,
1128 const gmx_mtop_t& top_global,
1129 const em_state_t* s_min,
1130 const em_state_t* s_b)
1134 fprintf(debug, "Doing reorder_partsum\n");
1137 auto fm = s_min->f.view().force();
1138 auto fb = s_b->f.view().force();
1140 /* Collect fm in a global vector fmg.
1141 * This conflicts with the spirit of domain decomposition,
1142 * but to fully optimize this a much more complicated algorithm is required.
1144 const int natoms = top_global.natoms;
1148 gmx::ArrayRef<const int> indicesMin = s_min->s.cg_gl;
1150 for (int a : indicesMin)
1152 copy_rvec(fm[i], fmg[a]);
1155 gmx_sum(top_global.natoms * 3, fmg[0], cr);
1157 /* Now we will determine the part of the sum for the cgs in state s_b */
1158 gmx::ArrayRef<const int> indicesB = s_b->s.cg_gl;
1163 gmx::ArrayRef<const unsigned char> grpnrFREEZE =
1164 top_global.groups.groupNumbers[SimulationAtomGroupType::Freeze];
1165 for (int a : indicesB)
1167 if (!grpnrFREEZE.empty())
1169 gf = grpnrFREEZE[i];
1171 for (int m = 0; m < DIM; m++)
1173 if (!opts->nFreeze[gf][m])
1175 partsum += (fb[i][m] - fmg[a][m]) * fb[i][m];
1186 //! Print some stuff, like beta, whatever that means.
1187 static real pr_beta(const t_commrec* cr,
1188 const t_grpopts* opts,
1190 const gmx_mtop_t& top_global,
1191 const em_state_t* s_min,
1192 const em_state_t* s_b)
1196 /* This is just the classical Polak-Ribiere calculation of beta;
1197 * it looks a bit complicated since we take freeze groups into account,
1198 * and might have to sum it in parallel runs.
1201 if (!DOMAINDECOMP(cr)
1202 || (s_min->s.ddp_count == cr->dd->ddp_count && s_b->s.ddp_count == cr->dd->ddp_count))
1204 auto fm = s_min->f.view().force();
1205 auto fb = s_b->f.view().force();
1208 /* This part of code can be incorrect with DD,
1209 * since the atom ordering in s_b and s_min might differ.
1211 for (int i = 0; i < mdatoms->homenr; i++)
1213 if (mdatoms->cFREEZE)
1215 gf = mdatoms->cFREEZE[i];
1217 for (int m = 0; m < DIM; m++)
1219 if (!opts->nFreeze[gf][m])
1221 sum += (fb[i][m] - fm[i][m]) * fb[i][m];
1228 /* We need to reorder cgs while summing */
1229 sum = reorder_partsum(cr, opts, top_global, s_min, s_b);
1233 gmx_sumd(1, &sum, cr);
1236 return sum / gmx::square(s_min->fnorm);
1242 void LegacySimulator::do_cg()
1244 const char* CG = "Polak-Ribiere Conjugate Gradients";
1246 gmx_localtop_t top(top_global.ffparams);
1247 gmx_global_stat_t gstat;
1248 double tmp, minstep;
1250 real a, b, c, beta = 0.0;
1253 gmx_bool converged, foundlower;
1254 rvec mu_tot = { 0 };
1255 gmx_bool do_log = FALSE, do_ene = FALSE, do_x, do_f;
1257 int number_steps, neval = 0, nstcg = inputrec->nstcgsteep;
1258 int m, step, nminstep;
1259 auto* mdatoms = mdAtoms->mdatoms();
1264 "Note that activating conjugate gradient energy minimization via the "
1265 "integrator .mdp option and the command gmx mdrun may "
1266 "be available in a different form in a future version of GROMACS, "
1267 "e.g. gmx minimize and an .mdp option.");
1273 // In CG, the state is extended with a search direction
1274 state_global->flags |= enumValueToBitMask(StateEntry::Cgp);
1276 // Ensure the extra per-atom state array gets allocated
1277 state_change_natoms(state_global, state_global->natoms);
1279 // Initialize the search direction to zero
1280 for (RVec& cg_p : state_global->cg_p)
1286 /* Create 4 states on the stack and extract pointers that we will swap */
1287 em_state_t s0{}, s1{}, s2{}, s3{};
1288 em_state_t* s_min = &s0;
1289 em_state_t* s_a = &s1;
1290 em_state_t* s_b = &s2;
1291 em_state_t* s_c = &s3;
1293 ObservablesReducer observablesReducer = observablesReducerBuilder->build();
1295 /* Init em and store the local state in s_min */
1314 const bool simulationsShareState = false;
1315 gmx_mdoutf* outf = init_mdoutf(fplog,
1326 StartingBehavior::NewSimulation,
1327 simulationsShareState,
1329 gmx::EnergyOutput energyOutput(mdoutf_get_fp_ene(outf),
1335 StartingBehavior::NewSimulation,
1336 simulationsShareState,
1337 mdModulesNotifiers);
1339 /* Print to log file */
1340 print_em_start(fplog, cr, walltime_accounting, wcycle, CG);
1342 /* Max number of steps */
1343 number_steps = inputrec->nsteps;
1347 sp_header(stderr, CG, inputrec->em_tol, number_steps);
1351 sp_header(fplog, CG, inputrec->em_tol, number_steps);
1354 EnergyEvaluator energyEvaluator{ fplog,
1366 &observablesReducer,
1375 /* Call the force routine and some auxiliary (neighboursearching etc.) */
1376 /* do_force always puts the charge groups in the box and shifts again
1377 * We do not unshift, so molecules are always whole in congrad.c
1379 energyEvaluator.run(s_min, mu_tot, vir, pres, -1, TRUE, step);
1383 /* Copy stuff to the energy bin for easy printing etc. */
1384 matrix nullBox = {};
1385 energyOutput.addDataAtEnergyStep(false,
1387 static_cast<double>(step),
1401 EnergyOutput::printHeader(fplog, step, step);
1402 energyOutput.printStepToEnergyFile(
1403 mdoutf_get_fp_ene(outf), TRUE, FALSE, FALSE, fplog, step, step, fr->fcdata.get(), nullptr);
1406 /* Estimate/guess the initial stepsize */
1407 stepsize = inputrec->em_stepsize / s_min->fnorm;
1411 double sqrtNumAtoms = sqrt(static_cast<double>(state_global->natoms));
1412 fprintf(stderr, " F-max = %12.5e on atom %d\n", s_min->fmax, s_min->a_fmax + 1);
1413 fprintf(stderr, " F-Norm = %12.5e\n", s_min->fnorm / sqrtNumAtoms);
1414 fprintf(stderr, "\n");
1415 /* and copy to the log file too... */
1416 fprintf(fplog, " F-max = %12.5e on atom %d\n", s_min->fmax, s_min->a_fmax + 1);
1417 fprintf(fplog, " F-Norm = %12.5e\n", s_min->fnorm / sqrtNumAtoms);
1418 fprintf(fplog, "\n");
1420 /* Start the loop over CG steps.
1421 * Each successful step is counted, and we continue until
1422 * we either converge or reach the max number of steps.
1425 for (step = 0; (number_steps < 0 || step <= number_steps) && !converged; step++)
1428 /* start taking steps in a new direction
1429 * First time we enter the routine, beta=0, and the direction is
1430 * simply the negative gradient.
1433 /* Calculate the new direction in p, and the gradient in this direction, gpa */
1434 gmx::ArrayRef<gmx::RVec> pm = s_min->s.cg_p;
1435 gmx::ArrayRef<const gmx::RVec> sfm = s_min->f.view().force();
1438 for (int i = 0; i < mdatoms->homenr; i++)
1440 if (mdatoms->cFREEZE)
1442 gf = mdatoms->cFREEZE[i];
1444 for (m = 0; m < DIM; m++)
1446 if (!inputrec->opts.nFreeze[gf][m])
1448 pm[i][m] = sfm[i][m] + beta * pm[i][m];
1449 gpa -= pm[i][m] * sfm[i][m];
1450 /* f is negative gradient, thus the sign */
1459 /* Sum the gradient along the line across CPUs */
1462 gmx_sumd(1, &gpa, cr);
1465 /* Calculate the norm of the search vector */
1466 get_f_norm_max(cr, &(inputrec->opts), mdatoms, pm, &pnorm, nullptr, nullptr);
1468 /* Just in case stepsize reaches zero due to numerical precision... */
1471 stepsize = inputrec->em_stepsize / pnorm;
1475 * Double check the value of the derivative in the search direction.
1476 * If it is positive it must be due to the old information in the
1477 * CG formula, so just remove that and start over with beta=0.
1478 * This corresponds to a steepest descent step.
1483 step--; /* Don't count this step since we are restarting */
1484 continue; /* Go back to the beginning of the big for-loop */
1487 /* Calculate minimum allowed stepsize, before the average (norm)
1488 * relative change in coordinate is smaller than precision
1491 auto s_min_x = makeArrayRef(s_min->s.x);
1492 for (int i = 0; i < mdatoms->homenr; i++)
1494 for (m = 0; m < DIM; m++)
1496 tmp = fabs(s_min_x[i][m]);
1501 tmp = pm[i][m] / tmp;
1502 minstep += tmp * tmp;
1505 /* Add up from all CPUs */
1508 gmx_sumd(1, &minstep, cr);
1511 minstep = GMX_REAL_EPS / sqrt(minstep / (3 * top_global.natoms));
1513 if (stepsize < minstep)
1519 /* Write coordinates if necessary */
1520 do_x = do_per_step(step, inputrec->nstxout);
1521 do_f = do_per_step(step, inputrec->nstfout);
1524 fplog, cr, outf, do_x, do_f, nullptr, top_global, inputrec, step, s_min, state_global, observablesHistory);
1526 /* Take a step downhill.
1527 * In theory, we should minimize the function along this direction.
1528 * That is quite possible, but it turns out to take 5-10 function evaluations
1529 * for each line. However, we dont really need to find the exact minimum -
1530 * it is much better to start a new CG step in a modified direction as soon
1531 * as we are close to it. This will save a lot of energy evaluations.
1533 * In practice, we just try to take a single step.
1534 * If it worked (i.e. lowered the energy), we increase the stepsize but
1535 * the continue straight to the next CG step without trying to find any minimum.
1536 * If it didn't work (higher energy), there must be a minimum somewhere between
1537 * the old position and the new one.
1539 * Due to the finite numerical accuracy, it turns out that it is a good idea
1540 * to even accept a SMALL increase in energy, if the derivative is still downhill.
1541 * This leads to lower final energies in the tests I've done. / Erik
1543 s_a->epot = s_min->epot;
1545 c = a + stepsize; /* reference position along line is zero */
1547 if (DOMAINDECOMP(cr) && s_min->s.ddp_count < cr->dd->ddp_count)
1549 em_dd_partition_system(fplog,
1567 /* Take a trial step (new coords in s_c) */
1568 do_em_step(cr, inputrec, mdatoms, s_min, c, s_min->s.cg_p.constArrayRefWithPadding(), s_c, constr, -1);
1571 /* Calculate energy for the trial step */
1572 energyEvaluator.run(s_c, mu_tot, vir, pres, -1, FALSE, step);
1574 /* Calc derivative along line */
1575 const rvec* pc = s_c->s.cg_p.rvec_array();
1576 gmx::ArrayRef<const gmx::RVec> sfc = s_c->f.view().force();
1578 for (int i = 0; i < mdatoms->homenr; i++)
1580 for (m = 0; m < DIM; m++)
1582 gpc -= pc[i][m] * sfc[i][m]; /* f is negative gradient, thus the sign */
1585 /* Sum the gradient along the line across CPUs */
1588 gmx_sumd(1, &gpc, cr);
1591 /* This is the max amount of increase in energy we tolerate */
1592 tmp = std::sqrt(GMX_REAL_EPS) * fabs(s_a->epot);
1594 /* Accept the step if the energy is lower, or if it is not significantly higher
1595 * and the line derivative is still negative.
1597 if (s_c->epot < s_a->epot || (gpc < 0 && s_c->epot < (s_a->epot + tmp)))
1600 /* Great, we found a better energy. Increase step for next iteration
1601 * if we are still going down, decrease it otherwise
1605 stepsize *= 1.618034; /* The golden section */
1609 stepsize *= 0.618034; /* 1/golden section */
1614 /* New energy is the same or higher. We will have to do some work
1615 * to find a smaller value in the interval. Take smaller step next time!
1618 stepsize *= 0.618034;
1622 /* OK, if we didn't find a lower value we will have to locate one now - there must
1623 * be one in the interval [a=0,c].
1624 * The same thing is valid here, though: Don't spend dozens of iterations to find
1625 * the line minimum. We try to interpolate based on the derivative at the endpoints,
1626 * and only continue until we find a lower value. In most cases this means 1-2 iterations.
1628 * I also have a safeguard for potentially really pathological functions so we never
1629 * take more than 20 steps before we give up ...
1631 * If we already found a lower value we just skip this step and continue to the update.
1640 /* Select a new trial point.
1641 * If the derivatives at points a & c have different sign we interpolate to zero,
1642 * otherwise just do a bisection.
1644 if (gpa < 0 && gpc > 0)
1646 b = a + gpa * (a - c) / (gpc - gpa);
1653 /* safeguard if interpolation close to machine accuracy causes errors:
1654 * never go outside the interval
1656 if (b <= a || b >= c)
1661 if (DOMAINDECOMP(cr) && s_min->s.ddp_count != cr->dd->ddp_count)
1663 /* Reload the old state */
1664 em_dd_partition_system(fplog,
1682 /* Take a trial step to this new point - new coords in s_b */
1683 do_em_step(cr, inputrec, mdatoms, s_min, b, s_min->s.cg_p.constArrayRefWithPadding(), s_b, constr, -1);
1686 /* Calculate energy for the trial step */
1687 energyEvaluator.run(s_b, mu_tot, vir, pres, -1, FALSE, step);
1689 /* p does not change within a step, but since the domain decomposition
1690 * might change, we have to use cg_p of s_b here.
1692 const rvec* pb = s_b->s.cg_p.rvec_array();
1693 gmx::ArrayRef<const gmx::RVec> sfb = s_b->f.view().force();
1695 for (int i = 0; i < mdatoms->homenr; i++)
1697 for (m = 0; m < DIM; m++)
1699 gpb -= pb[i][m] * sfb[i][m]; /* f is negative gradient, thus the sign */
1702 /* Sum the gradient along the line across CPUs */
1705 gmx_sumd(1, &gpb, cr);
1710 fprintf(debug, "CGE: EpotA %f EpotB %f EpotC %f gpb %f\n", s_a->epot, s_b->epot, s_c->epot, gpb);
1713 epot_repl = s_b->epot;
1715 /* Keep one of the intervals based on the value of the derivative at the new point */
1718 /* Replace c endpoint with b */
1719 swap_em_state(&s_b, &s_c);
1725 /* Replace a endpoint with b */
1726 swap_em_state(&s_b, &s_a);
1732 * Stop search as soon as we find a value smaller than the endpoints.
1733 * Never run more than 20 steps, no matter what.
1736 } while ((epot_repl > s_a->epot || epot_repl > s_c->epot) && (nminstep < 20));
1738 if (std::fabs(epot_repl - s_min->epot) < fabs(s_min->epot) * GMX_REAL_EPS || nminstep >= 20)
1740 /* OK. We couldn't find a significantly lower energy.
1741 * If beta==0 this was steepest descent, and then we give up.
1742 * If not, set beta=0 and restart with steepest descent before quitting.
1752 /* Reset memory before giving up */
1758 /* Select min energy state of A & C, put the best in B.
1760 if (s_c->epot < s_a->epot)
1764 fprintf(debug, "CGE: C (%f) is lower than A (%f), moving C to B\n", s_c->epot, s_a->epot);
1766 swap_em_state(&s_b, &s_c);
1773 fprintf(debug, "CGE: A (%f) is lower than C (%f), moving A to B\n", s_a->epot, s_c->epot);
1775 swap_em_state(&s_b, &s_a);
1783 fprintf(debug, "CGE: Found a lower energy %f, moving C to B\n", s_c->epot);
1785 swap_em_state(&s_b, &s_c);
1789 /* new search direction */
1790 /* beta = 0 means forget all memory and restart with steepest descents. */
1791 if (nstcg && ((step % nstcg) == 0))
1797 /* s_min->fnorm cannot be zero, because then we would have converged
1801 /* Polak-Ribiere update.
1802 * Change to fnorm2/fnorm2_old for Fletcher-Reeves
1804 beta = pr_beta(cr, &inputrec->opts, mdatoms, top_global, s_min, s_b);
1806 /* Limit beta to prevent oscillations */
1807 if (fabs(beta) > 5.0)
1813 /* update positions */
1814 swap_em_state(&s_min, &s_b);
1817 /* Print it if necessary */
1820 if (mdrunOptions.verbose)
1822 double sqrtNumAtoms = sqrt(static_cast<double>(state_global->natoms));
1824 "\rStep %d, Epot=%12.6e, Fnorm=%9.3e, Fmax=%9.3e (atom %d)\n",
1827 s_min->fnorm / sqrtNumAtoms,
1832 /* Store the new (lower) energies */
1833 matrix nullBox = {};
1834 energyOutput.addDataAtEnergyStep(false,
1836 static_cast<double>(step),
1850 do_log = do_per_step(step, inputrec->nstlog);
1851 do_ene = do_per_step(step, inputrec->nstenergy);
1853 imdSession->fillEnergyRecord(step, TRUE);
1857 EnergyOutput::printHeader(fplog, step, step);
1859 energyOutput.printStepToEnergyFile(mdoutf_get_fp_ene(outf),
1863 do_log ? fplog : nullptr,
1870 /* Send energies and positions to the IMD client if bIMD is TRUE. */
1871 if (MASTER(cr) && imdSession->run(step, TRUE, state_global->box, state_global->x, 0))
1873 imdSession->sendPositionsAndEnergies();
1876 /* Stop when the maximum force lies below tolerance.
1877 * If we have reached machine precision, converged is already set to true.
1879 converged = converged || (s_min->fmax < inputrec->em_tol);
1881 } /* End of the loop */
1885 step--; /* we never took that last step in this case */
1887 if (s_min->fmax > inputrec->em_tol)
1891 warn_step(fplog, inputrec->em_tol, s_min->fmax, step - 1 == number_steps, FALSE);
1898 /* If we printed energy and/or logfile last step (which was the last step)
1899 * we don't have to do it again, but otherwise print the final values.
1903 /* Write final value to log since we didn't do anything the last step */
1904 EnergyOutput::printHeader(fplog, step, step);
1906 if (!do_ene || !do_log)
1908 /* Write final energy file entries */
1909 energyOutput.printStepToEnergyFile(mdoutf_get_fp_ene(outf),
1913 !do_log ? fplog : nullptr,
1921 /* Print some stuff... */
1924 fprintf(stderr, "\nwriting lowest energy coordinates.\n");
1928 * For accurate normal mode calculation it is imperative that we
1929 * store the last conformation into the full precision binary trajectory.
1931 * However, we should only do it if we did NOT already write this step
1932 * above (which we did if do_x or do_f was true).
1934 /* Note that with 0 < nstfout != nstxout we can end up with two frames
1935 * in the trajectory with the same step number.
1937 do_x = !do_per_step(step, inputrec->nstxout);
1938 do_f = (inputrec->nstfout > 0 && !do_per_step(step, inputrec->nstfout));
1941 fplog, cr, outf, do_x, do_f, ftp2fn(efSTO, nfile, fnm), top_global, inputrec, step, s_min, state_global, observablesHistory);
1946 double sqrtNumAtoms = sqrt(static_cast<double>(state_global->natoms));
1947 print_converged(stderr, CG, inputrec->em_tol, step, converged, number_steps, s_min, sqrtNumAtoms);
1948 print_converged(fplog, CG, inputrec->em_tol, step, converged, number_steps, s_min, sqrtNumAtoms);
1950 fprintf(fplog, "\nPerformed %d energy evaluations in total.\n", neval);
1953 finish_em(cr, outf, walltime_accounting, wcycle);
1955 /* To print the actual number of steps we needed somewhere */
1956 walltime_accounting_set_nsteps_done(walltime_accounting, step);
1960 void LegacySimulator::do_lbfgs()
1962 static const char* LBFGS = "Low-Memory BFGS Minimizer";
1964 gmx_localtop_t top(top_global.ffparams);
1965 gmx_global_stat_t gstat;
1966 auto* mdatoms = mdAtoms->mdatoms();
1971 "Note that activating L-BFGS energy minimization via the "
1972 "integrator .mdp option and the command gmx mdrun may "
1973 "be available in a different form in a future version of GROMACS, "
1974 "e.g. gmx minimize and an .mdp option.");
1978 gmx_fatal(FARGS, "L-BFGS minimization only supports a single rank");
1981 if (nullptr != constr)
1985 "The combination of constraints and L-BFGS minimization is not implemented. Either "
1986 "do not use constraints, or use another minimizer (e.g. steepest descent).");
1989 const int n = 3 * state_global->natoms;
1990 const int nmaxcorr = inputrec->nbfgscorr;
1992 std::vector<real> p(n);
1993 std::vector<real> rho(nmaxcorr);
1994 std::vector<real> alpha(nmaxcorr);
1996 std::vector<std::vector<real>> dx(nmaxcorr);
1997 for (auto& dxCorr : dx)
2002 std::vector<std::vector<real>> dg(nmaxcorr);
2003 for (auto& dgCorr : dg)
2011 ObservablesReducer observablesReducer = observablesReducerBuilder->build();
2032 const bool simulationsShareState = false;
2033 gmx_mdoutf* outf = init_mdoutf(fplog,
2044 StartingBehavior::NewSimulation,
2045 simulationsShareState,
2047 gmx::EnergyOutput energyOutput(mdoutf_get_fp_ene(outf),
2053 StartingBehavior::NewSimulation,
2054 simulationsShareState,
2055 mdModulesNotifiers);
2057 const int start = 0;
2058 const int end = mdatoms->homenr;
2060 /* We need 4 working states */
2061 em_state_t s0{}, s1{}, s2{}, s3{};
2062 em_state_t* sa = &s0;
2063 em_state_t* sb = &s1;
2064 em_state_t* sc = &s2;
2065 em_state_t* last = &s3;
2066 /* Initialize by copying the state from ems (we could skip x and f here) */
2071 /* Print to log file */
2072 print_em_start(fplog, cr, walltime_accounting, wcycle, LBFGS);
2074 /* Max number of steps */
2075 const int number_steps = inputrec->nsteps;
2077 /* Create a 3*natoms index to tell whether each degree of freedom is frozen */
2078 std::vector<bool> frozen(n);
2080 for (int i = start; i < end; i++)
2082 if (mdatoms->cFREEZE)
2084 gf = mdatoms->cFREEZE[i];
2086 for (int m = 0; m < DIM; m++)
2088 frozen[3 * i + m] = (inputrec->opts.nFreeze[gf][m] != 0);
2093 sp_header(stderr, LBFGS, inputrec->em_tol, number_steps);
2097 sp_header(fplog, LBFGS, inputrec->em_tol, number_steps);
2102 vsite->construct(state_global->x, {}, state_global->box, VSiteOperation::Positions);
2105 /* Call the force routine and some auxiliary (neighboursearching etc.) */
2106 /* do_force always puts the charge groups in the box and shifts again
2107 * We do not unshift, so molecules are always whole
2110 EnergyEvaluator energyEvaluator{ fplog,
2122 &observablesReducer,
2132 energyEvaluator.run(&ems, mu_tot, vir, pres, -1, TRUE, step);
2136 /* Copy stuff to the energy bin for easy printing etc. */
2137 matrix nullBox = {};
2138 energyOutput.addDataAtEnergyStep(false,
2140 static_cast<double>(step),
2154 EnergyOutput::printHeader(fplog, step, step);
2155 energyOutput.printStepToEnergyFile(
2156 mdoutf_get_fp_ene(outf), TRUE, FALSE, FALSE, fplog, step, step, fr->fcdata.get(), nullptr);
2159 /* Set the initial step.
2160 * since it will be multiplied by the non-normalized search direction
2161 * vector (force vector the first time), we scale it by the
2162 * norm of the force.
2167 double sqrtNumAtoms = sqrt(static_cast<double>(state_global->natoms));
2168 fprintf(stderr, "Using %d BFGS correction steps.\n\n", nmaxcorr);
2169 fprintf(stderr, " F-max = %12.5e on atom %d\n", ems.fmax, ems.a_fmax + 1);
2170 fprintf(stderr, " F-Norm = %12.5e\n", ems.fnorm / sqrtNumAtoms);
2171 fprintf(stderr, "\n");
2172 /* and copy to the log file too... */
2173 fprintf(fplog, "Using %d BFGS correction steps.\n\n", nmaxcorr);
2174 fprintf(fplog, " F-max = %12.5e on atom %d\n", ems.fmax, ems.a_fmax + 1);
2175 fprintf(fplog, " F-Norm = %12.5e\n", ems.fnorm / sqrtNumAtoms);
2176 fprintf(fplog, "\n");
2179 // Point is an index to the memory of search directions, where 0 is the first one.
2182 // Set initial search direction to the force (-gradient), or 0 for frozen particles.
2183 real* fInit = static_cast<real*>(ems.f.view().force().data()[0]);
2184 for (int i = 0; i < n; i++)
2188 dx[point][i] = fInit[i]; /* Initial search direction */
2196 // Stepsize will be modified during the search, and actually it is not critical
2197 // (the main efficiency in the algorithm comes from changing directions), but
2198 // we still need an initial value, so estimate it as the inverse of the norm
2199 // so we take small steps where the potential fluctuates a lot.
2200 double stepsize = 1.0 / ems.fnorm;
2202 /* Start the loop over BFGS steps.
2203 * Each successful step is counted, and we continue until
2204 * we either converge or reach the max number of steps.
2212 /* Set the gradient from the force */
2213 bool converged = false;
2214 for (int step = 0; (number_steps < 0 || step <= number_steps) && !converged; step++)
2217 /* Write coordinates if necessary */
2218 const bool do_x = do_per_step(step, inputrec->nstxout);
2219 const bool do_f = do_per_step(step, inputrec->nstfout);
2224 mdof_flags |= MDOF_X;
2229 mdof_flags |= MDOF_F;
2234 mdof_flags |= MDOF_IMD;
2237 gmx::WriteCheckpointDataHolder checkpointDataHolder;
2238 mdoutf_write_to_trajectory_files(fplog,
2244 static_cast<real>(step),
2248 ems.f.view().force(),
2249 &checkpointDataHolder);
2251 /* Do the linesearching in the direction dx[point][0..(n-1)] */
2253 /* make s a pointer to current search direction - point=0 first time we get here */
2254 gmx::ArrayRef<const real> s = dx[point];
2256 const real* xx = static_cast<real*>(ems.s.x.rvec_array()[0]);
2257 const real* ff = static_cast<real*>(ems.f.view().force().data()[0]);
2259 // calculate line gradient in position A
2261 for (int i = 0; i < n; i++)
2263 gpa -= s[i] * ff[i];
2266 /* Calculate minimum allowed stepsize along the line, before the average (norm)
2267 * relative change in coordinate is smaller than precision
2270 for (int i = 0; i < n; i++)
2272 double tmp = fabs(xx[i]);
2278 minstep += tmp * tmp;
2280 minstep = GMX_REAL_EPS / sqrt(minstep / n);
2282 if (stepsize < minstep)
2288 // Before taking any steps along the line, store the old position
2290 real* lastx = static_cast<real*>(last->s.x.data()[0]);
2291 real* lastf = static_cast<real*>(last->f.view().force().data()[0]);
2292 const real Epot0 = ems.epot;
2296 /* Take a step downhill.
2297 * In theory, we should find the actual minimum of the function in this
2298 * direction, somewhere along the line.
2299 * That is quite possible, but it turns out to take 5-10 function evaluations
2300 * for each line. However, we dont really need to find the exact minimum -
2301 * it is much better to start a new BFGS step in a modified direction as soon
2302 * as we are close to it. This will save a lot of energy evaluations.
2304 * In practice, we just try to take a single step.
2305 * If it worked (i.e. lowered the energy), we increase the stepsize but
2306 * continue straight to the next BFGS step without trying to find any minimum,
2307 * i.e. we change the search direction too. If the line was smooth, it is
2308 * likely we are in a smooth region, and then it makes sense to take longer
2309 * steps in the modified search direction too.
2311 * If it didn't work (higher energy), there must be a minimum somewhere between
2312 * the old position and the new one. Then we need to start by finding a lower
2313 * value before we change search direction. Since the energy was apparently
2314 * quite rough, we need to decrease the step size.
2316 * Due to the finite numerical accuracy, it turns out that it is a good idea
2317 * to accept a SMALL increase in energy, if the derivative is still downhill.
2318 * This leads to lower final energies in the tests I've done. / Erik
2321 // State "A" is the first position along the line.
2322 // reference position along line is initially zero
2325 // Check stepsize first. We do not allow displacements
2326 // larger than emstep.
2332 // Pick a new position C by adding stepsize to A.
2335 // Calculate what the largest change in any individual coordinate
2336 // would be (translation along line * gradient along line)
2338 for (int i = 0; i < n; i++)
2340 real delta = c * s[i];
2341 if (delta > maxdelta)
2346 // If any displacement is larger than the stepsize limit, reduce the step
2347 if (maxdelta > inputrec->em_stepsize)
2351 } while (maxdelta > inputrec->em_stepsize);
2353 // Take a trial step and move the coordinate array xc[] to position C
2354 real* xc = static_cast<real*>(sc->s.x.rvec_array()[0]);
2355 for (int i = 0; i < n; i++)
2357 xc[i] = lastx[i] + c * s[i];
2361 // Calculate energy for the trial step in position C
2362 energyEvaluator.run(sc, mu_tot, vir, pres, step, FALSE, step);
2364 // Calc line gradient in position C
2365 real* fc = static_cast<real*>(sc->f.view().force()[0]);
2367 for (int i = 0; i < n; i++)
2369 gpc -= s[i] * fc[i]; /* f is negative gradient, thus the sign */
2371 /* Sum the gradient along the line across CPUs */
2374 gmx_sumd(1, &gpc, cr);
2377 // This is the max amount of increase in energy we tolerate.
2378 // By allowing VERY small changes (close to numerical precision) we
2379 // frequently find even better (lower) final energies.
2380 double tmp = std::sqrt(GMX_REAL_EPS) * fabs(sa->epot);
2382 // Accept the step if the energy is lower in the new position C (compared to A),
2383 // or if it is not significantly higher and the line derivative is still negative.
2384 bool foundlower = sc->epot < sa->epot || (gpc < 0 && sc->epot < (sa->epot + tmp));
2385 // If true, great, we found a better energy. We no longer try to alter the
2386 // stepsize, but simply accept this new better position. The we select a new
2387 // search direction instead, which will be much more efficient than continuing
2388 // to take smaller steps along a line. Set fnorm based on the new C position,
2389 // which will be used to update the stepsize to 1/fnorm further down.
2391 // If false, the energy is NOT lower in point C, i.e. it will be the same
2392 // or higher than in point A. In this case it is pointless to move to point C,
2393 // so we will have to do more iterations along the same line to find a smaller
2394 // value in the interval [A=0.0,C].
2395 // Here, A is still 0.0, but that will change when we do a search in the interval
2396 // [0.0,C] below. That search we will do by interpolation or bisection rather
2397 // than with the stepsize, so no need to modify it. For the next search direction
2398 // it will be reset to 1/fnorm anyway.
2403 // OK, if we didn't find a lower value we will have to locate one now - there must
2404 // be one in the interval [a,c].
2405 // The same thing is valid here, though: Don't spend dozens of iterations to find
2406 // the line minimum. We try to interpolate based on the derivative at the endpoints,
2407 // and only continue until we find a lower value. In most cases this means 1-2 iterations.
2408 // I also have a safeguard for potentially really pathological functions so we never
2409 // take more than 20 steps before we give up.
2410 // If we already found a lower value we just skip this step and continue to the update.
2415 // Select a new trial point B in the interval [A,C].
2416 // If the derivatives at points a & c have different sign we interpolate to zero,
2417 // otherwise just do a bisection since there might be multiple minima/maxima
2418 // inside the interval.
2420 if (gpa < 0 && gpc > 0)
2422 b = a + gpa * (a - c) / (gpc - gpa);
2429 /* safeguard if interpolation close to machine accuracy causes errors:
2430 * never go outside the interval
2432 if (b <= a || b >= c)
2437 // Take a trial step to point B
2438 real* xb = static_cast<real*>(sb->s.x.rvec_array()[0]);
2439 for (int i = 0; i < n; i++)
2441 xb[i] = lastx[i] + b * s[i];
2445 // Calculate energy for the trial step in point B
2446 energyEvaluator.run(sb, mu_tot, vir, pres, step, FALSE, step);
2449 // Calculate gradient in point B
2450 real* fb = static_cast<real*>(sb->f.view().force()[0]);
2452 for (int i = 0; i < n; i++)
2454 gpb -= s[i] * fb[i]; /* f is negative gradient, thus the sign */
2456 /* Sum the gradient along the line across CPUs */
2459 gmx_sumd(1, &gpb, cr);
2462 // Keep one of the intervals [A,B] or [B,C] based on the value of the derivative
2463 // at the new point B, and rename the endpoints of this new interval A and C.
2466 /* Replace c endpoint with b */
2468 /* copy state b to c */
2473 /* Replace a endpoint with b */
2475 /* copy state b to a */
2480 * Stop search as soon as we find a value smaller than the endpoints,
2481 * or if the tolerance is below machine precision.
2482 * Never run more than 20 steps, no matter what.
2485 } while ((sb->epot > sa->epot || sb->epot > sc->epot) && (nminstep < 20));
2487 if (std::fabs(sb->epot - Epot0) < GMX_REAL_EPS || nminstep >= 20)
2489 /* OK. We couldn't find a significantly lower energy.
2490 * If ncorr==0 this was steepest descent, and then we give up.
2491 * If not, reset memory to restart as steepest descent before quitting.
2503 /* Search in gradient direction */
2504 for (int i = 0; i < n; i++)
2506 dx[point][i] = ff[i];
2508 /* Reset stepsize */
2509 stepsize = 1.0 / fnorm;
2514 /* Select min energy state of A & C, put the best in xx/ff/Epot
2516 if (sc->epot < sa->epot)
2537 /* Update the memory information, and calculate a new
2538 * approximation of the inverse hessian
2541 /* Have new data in Epot, xx, ff */
2542 if (ncorr < nmaxcorr)
2547 for (int i = 0; i < n; i++)
2549 dg[point][i] = lastf[i] - ff[i];
2550 dx[point][i] *= step_taken;
2555 for (int i = 0; i < n; i++)
2557 dgdg += dg[point][i] * dg[point][i];
2558 dgdx += dg[point][i] * dx[point][i];
2561 const real diag = dgdx / dgdg;
2563 rho[point] = 1.0 / dgdx;
2566 if (point >= nmaxcorr)
2572 for (int i = 0; i < n; i++)
2579 /* Recursive update. First go back over the memory points */
2580 for (int k = 0; k < ncorr; k++)
2589 for (int i = 0; i < n; i++)
2591 sq += dx[cp][i] * p[i];
2594 alpha[cp] = rho[cp] * sq;
2596 for (int i = 0; i < n; i++)
2598 p[i] -= alpha[cp] * dg[cp][i];
2602 for (int i = 0; i < n; i++)
2607 /* And then go forward again */
2608 for (int k = 0; k < ncorr; k++)
2611 for (int i = 0; i < n; i++)
2613 yr += p[i] * dg[cp][i];
2616 real beta = rho[cp] * yr;
2617 beta = alpha[cp] - beta;
2619 for (int i = 0; i < n; i++)
2621 p[i] += beta * dx[cp][i];
2631 for (int i = 0; i < n; i++)
2635 dx[point][i] = p[i];
2643 /* Print it if necessary */
2646 if (mdrunOptions.verbose)
2648 double sqrtNumAtoms = sqrt(static_cast<double>(state_global->natoms));
2650 "\rStep %d, Epot=%12.6e, Fnorm=%9.3e, Fmax=%9.3e (atom %d)\n",
2653 ems.fnorm / sqrtNumAtoms,
2658 /* Store the new (lower) energies */
2659 matrix nullBox = {};
2660 energyOutput.addDataAtEnergyStep(false,
2662 static_cast<double>(step),
2676 do_log = do_per_step(step, inputrec->nstlog);
2677 do_ene = do_per_step(step, inputrec->nstenergy);
2679 imdSession->fillEnergyRecord(step, TRUE);
2683 EnergyOutput::printHeader(fplog, step, step);
2685 energyOutput.printStepToEnergyFile(mdoutf_get_fp_ene(outf),
2689 do_log ? fplog : nullptr,
2696 /* Send x and E to IMD client, if bIMD is TRUE. */
2697 if (imdSession->run(step, TRUE, state_global->box, state_global->x, 0) && MASTER(cr))
2699 imdSession->sendPositionsAndEnergies();
2702 // Reset stepsize in we are doing more iterations
2705 /* Stop when the maximum force lies below tolerance.
2706 * If we have reached machine precision, converged is already set to true.
2708 converged = converged || (ems.fmax < inputrec->em_tol);
2710 } /* End of the loop */
2714 step--; /* we never took that last step in this case */
2716 if (ems.fmax > inputrec->em_tol)
2720 warn_step(fplog, inputrec->em_tol, ems.fmax, step - 1 == number_steps, FALSE);
2725 /* If we printed energy and/or logfile last step (which was the last step)
2726 * we don't have to do it again, but otherwise print the final values.
2728 if (!do_log) /* Write final value to log since we didn't do anythin last step */
2730 EnergyOutput::printHeader(fplog, step, step);
2732 if (!do_ene || !do_log) /* Write final energy file entries */
2734 energyOutput.printStepToEnergyFile(mdoutf_get_fp_ene(outf),
2738 !do_log ? fplog : nullptr,
2745 /* Print some stuff... */
2748 fprintf(stderr, "\nwriting lowest energy coordinates.\n");
2752 * For accurate normal mode calculation it is imperative that we
2753 * store the last conformation into the full precision binary trajectory.
2755 * However, we should only do it if we did NOT already write this step
2756 * above (which we did if do_x or do_f was true).
2758 const bool do_x = !do_per_step(step, inputrec->nstxout);
2759 const bool do_f = !do_per_step(step, inputrec->nstfout);
2761 fplog, cr, outf, do_x, do_f, ftp2fn(efSTO, nfile, fnm), top_global, inputrec, step, &ems, state_global, observablesHistory);
2765 double sqrtNumAtoms = sqrt(static_cast<double>(state_global->natoms));
2766 print_converged(stderr, LBFGS, inputrec->em_tol, step, converged, number_steps, &ems, sqrtNumAtoms);
2767 print_converged(fplog, LBFGS, inputrec->em_tol, step, converged, number_steps, &ems, sqrtNumAtoms);
2769 fprintf(fplog, "\nPerformed %d energy evaluations in total.\n", neval);
2772 finish_em(cr, outf, walltime_accounting, wcycle);
2774 /* To print the actual number of steps we needed somewhere */
2775 walltime_accounting_set_nsteps_done(walltime_accounting, step);
2778 void LegacySimulator::do_steep()
2780 const char* SD = "Steepest Descents";
2781 gmx_localtop_t top(top_global.ffparams);
2782 gmx_global_stat_t gstat;
2785 gmx_bool bDone, bAbort, do_x, do_f;
2787 rvec mu_tot = { 0 };
2790 int steps_accepted = 0;
2791 auto* mdatoms = mdAtoms->mdatoms();
2796 "Note that activating steepest-descent energy minimization via the "
2797 "integrator .mdp option and the command gmx mdrun may "
2798 "be available in a different form in a future version of GROMACS, "
2799 "e.g. gmx minimize and an .mdp option.");
2801 /* Create 2 states on the stack and extract pointers that we will swap */
2802 em_state_t s0{}, s1{};
2803 em_state_t* s_min = &s0;
2804 em_state_t* s_try = &s1;
2806 ObservablesReducer observablesReducer = observablesReducerBuilder->build();
2808 /* Init em and store the local state in s_try */
2827 const bool simulationsShareState = false;
2828 gmx_mdoutf* outf = init_mdoutf(fplog,
2839 StartingBehavior::NewSimulation,
2840 simulationsShareState,
2842 gmx::EnergyOutput energyOutput(mdoutf_get_fp_ene(outf),
2848 StartingBehavior::NewSimulation,
2849 simulationsShareState,
2850 mdModulesNotifiers);
2852 /* Print to log file */
2853 print_em_start(fplog, cr, walltime_accounting, wcycle, SD);
2855 /* Set variables for stepsize (in nm). This is the largest
2856 * step that we are going to make in any direction.
2858 ustep = inputrec->em_stepsize;
2861 /* Max number of steps */
2862 nsteps = inputrec->nsteps;
2866 /* Print to the screen */
2867 sp_header(stderr, SD, inputrec->em_tol, nsteps);
2871 sp_header(fplog, SD, inputrec->em_tol, nsteps);
2873 EnergyEvaluator energyEvaluator{ fplog,
2885 &observablesReducer,
2893 /**** HERE STARTS THE LOOP ****
2894 * count is the counter for the number of steps
2895 * bDone will be TRUE when the minimization has converged
2896 * bAbort will be TRUE when nsteps steps have been performed or when
2897 * the stepsize becomes smaller than is reasonable for machine precision
2902 while (!bDone && !bAbort)
2904 bAbort = (nsteps >= 0) && (count == nsteps);
2906 /* set new coordinates, except for first step */
2907 bool validStep = true;
2910 validStep = do_em_step(
2911 cr, inputrec, mdatoms, s_min, stepsize, s_min->f.view().forceWithPadding(), s_try, constr, count);
2916 energyEvaluator.run(s_try, mu_tot, vir, pres, count, count == 0, count);
2920 // Signal constraint error during stepping with energy=inf
2921 s_try->epot = std::numeric_limits<real>::infinity();
2926 EnergyOutput::printHeader(fplog, count, count);
2931 s_min->epot = s_try->epot;
2934 /* Print it if necessary */
2937 if (mdrunOptions.verbose)
2940 "Step=%5d, Dmax= %6.1e nm, Epot= %12.5e Fmax= %11.5e, atom= %d%c",
2946 ((count == 0) || (s_try->epot < s_min->epot)) ? '\n' : '\r');
2950 if ((count == 0) || (s_try->epot < s_min->epot))
2952 /* Store the new (lower) energies */
2953 matrix nullBox = {};
2954 energyOutput.addDataAtEnergyStep(false,
2956 static_cast<double>(count),
2970 imdSession->fillEnergyRecord(count, TRUE);
2972 const bool do_dr = do_per_step(steps_accepted, inputrec->nstdisreout);
2973 const bool do_or = do_per_step(steps_accepted, inputrec->nstorireout);
2974 energyOutput.printStepToEnergyFile(
2975 mdoutf_get_fp_ene(outf), TRUE, do_dr, do_or, fplog, count, count, fr->fcdata.get(), nullptr);
2980 /* Now if the new energy is smaller than the previous...
2981 * or if this is the first step!
2982 * or if we did random steps!
2985 if ((count == 0) || (s_try->epot < s_min->epot))
2989 /* Test whether the convergence criterion is met... */
2990 bDone = (s_try->fmax < inputrec->em_tol);
2992 /* Copy the arrays for force, positions and energy */
2993 /* The 'Min' array always holds the coords and forces of the minimal
2995 swap_em_state(&s_min, &s_try);
3001 /* Write to trn, if necessary */
3002 do_x = do_per_step(steps_accepted, inputrec->nstxout);
3003 do_f = do_per_step(steps_accepted, inputrec->nstfout);
3005 fplog, cr, outf, do_x, do_f, nullptr, top_global, inputrec, count, s_min, state_global, observablesHistory);
3009 /* If energy is not smaller make the step smaller... */
3012 if (DOMAINDECOMP(cr) && s_min->s.ddp_count != cr->dd->ddp_count)
3014 /* Reload the old state */
3015 em_dd_partition_system(fplog,
3034 // If the force is very small after finishing minimization,
3035 // we risk dividing by zero when calculating the step size.
3036 // So we check first if the minimization has stopped before
3037 // trying to obtain a new step size.
3040 /* Determine new step */
3041 stepsize = ustep / s_min->fmax;
3044 /* Check if stepsize is too small, with 1 nm as a characteristic length */
3046 if (count == nsteps || ustep < 1e-12)
3048 if (count == nsteps || ustep < 1e-6)
3053 warn_step(fplog, inputrec->em_tol, s_min->fmax, count == nsteps, constr != nullptr);
3058 /* Send IMD energies and positions, if bIMD is TRUE. */
3059 if (imdSession->run(count,
3061 MASTER(cr) ? state_global->box : nullptr,
3062 MASTER(cr) ? state_global->x : gmx::ArrayRef<gmx::RVec>(),
3066 imdSession->sendPositionsAndEnergies();
3070 } /* End of the loop */
3072 /* Print some data... */
3075 fprintf(stderr, "\nwriting lowest energy coordinates.\n");
3077 write_em_traj(fplog,
3081 inputrec->nstfout != 0,
3082 ftp2fn(efSTO, nfile, fnm),
3088 observablesHistory);
3092 double sqrtNumAtoms = sqrt(static_cast<double>(state_global->natoms));
3094 print_converged(stderr, SD, inputrec->em_tol, count, bDone, nsteps, s_min, sqrtNumAtoms);
3095 print_converged(fplog, SD, inputrec->em_tol, count, bDone, nsteps, s_min, sqrtNumAtoms);
3098 finish_em(cr, outf, walltime_accounting, wcycle);
3100 /* To print the actual number of steps we needed somewhere */
3102 // TODO: Avoid changing inputrec (#3854)
3103 auto* nonConstInputrec = const_cast<t_inputrec*>(inputrec);
3104 nonConstInputrec->nsteps = count;
3107 walltime_accounting_set_nsteps_done(walltime_accounting, count);
3110 void LegacySimulator::do_nm()
3112 const char* NM = "Normal Mode Analysis";
3114 gmx_localtop_t top(top_global.ffparams);
3115 gmx_global_stat_t gstat;
3117 rvec mu_tot = { 0 };
3119 gmx_bool bSparse; /* use sparse matrix storage format */
3121 gmx_sparsematrix_t* sparse_matrix = nullptr;
3122 real* full_matrix = nullptr;
3124 /* added with respect to mdrun */
3126 real der_range = 10.0 * std::sqrt(GMX_REAL_EPS);
3128 bool bIsMaster = MASTER(cr);
3129 auto* mdatoms = mdAtoms->mdatoms();
3134 "Note that activating normal-mode analysis via the integrator "
3135 ".mdp option and the command gmx mdrun may "
3136 "be available in a different form in a future version of GROMACS, "
3137 "e.g. gmx normal-modes.");
3139 if (constr != nullptr)
3143 "Constraints present with Normal Mode Analysis, this combination is not supported");
3146 gmx_shellfc_t* shellfc;
3148 em_state_t state_work{};
3150 ObservablesReducer observablesReducer = observablesReducerBuilder->build();
3152 /* Init em and store the local state in state_minimum */
3171 const bool simulationsShareState = false;
3172 gmx_mdoutf* outf = init_mdoutf(fplog,
3183 StartingBehavior::NewSimulation,
3184 simulationsShareState,
3187 std::vector<int> atom_index = get_atom_index(top_global);
3188 std::vector<gmx::RVec> fneg(atom_index.size(), { 0, 0, 0 });
3189 snew(dfdx, atom_index.size());
3195 "NOTE: This version of GROMACS has been compiled in single precision,\n"
3196 " which MIGHT not be accurate enough for normal mode analysis.\n"
3197 " GROMACS now uses sparse matrix storage, so the memory requirements\n"
3198 " are fairly modest even if you recompile in double precision.\n\n");
3202 /* Check if we can/should use sparse storage format.
3204 * Sparse format is only useful when the Hessian itself is sparse, which it
3205 * will be when we use a cutoff.
3206 * For small systems (n<1000) it is easier to always use full matrix format, though.
3208 if (EEL_FULL(fr->ic->eeltype) || fr->rlist == 0.0)
3210 GMX_LOG(mdlog.warning)
3211 .appendText("Non-cutoff electrostatics used, forcing full Hessian format.");
3214 else if (atom_index.size() < 1000)
3216 GMX_LOG(mdlog.warning)
3217 .appendTextFormatted("Small system size (N=%zu), using full Hessian format.",
3223 GMX_LOG(mdlog.warning).appendText("Using compressed symmetric sparse Hessian format.");
3227 /* Number of dimensions, based on real atoms, that is not vsites or shell */
3228 sz = DIM * atom_index.size();
3230 fprintf(stderr, "Allocating Hessian memory...\n\n");
3234 sparse_matrix = gmx_sparsematrix_init(sz);
3235 sparse_matrix->compressed_symmetric = TRUE;
3239 snew(full_matrix, sz * sz);
3242 /* Write start time and temperature */
3243 print_em_start(fplog, cr, walltime_accounting, wcycle, NM);
3245 /* fudge nr of steps to nr of atoms */
3247 // TODO: Avoid changing inputrec (#3854)
3248 auto* nonConstInputrec = const_cast<t_inputrec*>(inputrec);
3249 nonConstInputrec->nsteps = atom_index.size() * 2;
3255 "starting normal mode calculation '%s'\n%" PRId64 " steps.\n\n",
3260 nnodes = cr->nnodes;
3262 /* Make evaluate_energy do a single node force calculation */
3264 EnergyEvaluator energyEvaluator{ fplog,
3276 &observablesReducer,
3283 energyEvaluator.run(&state_work, mu_tot, vir, pres, -1, TRUE, 0);
3284 cr->nnodes = nnodes;
3286 /* if forces are not small, warn user */
3287 get_state_f_norm_max(cr, &(inputrec->opts), mdatoms, &state_work);
3289 GMX_LOG(mdlog.warning).appendTextFormatted("Maximum force:%12.5e", state_work.fmax);
3290 if (state_work.fmax > 1.0e-3)
3292 GMX_LOG(mdlog.warning)
3294 "The force is probably not small enough to "
3295 "ensure that you are at a minimum.\n"
3296 "Be aware that negative eigenvalues may occur\n"
3297 "when the resulting matrix is diagonalized.");
3300 /***********************************************************
3302 * Loop over all pairs in matrix
3304 * do_force called twice. Once with positive and
3305 * once with negative displacement
3307 ************************************************************/
3309 /* Steps are divided one by one over the nodes */
3311 auto state_work_x = makeArrayRef(state_work.s.x);
3312 auto state_work_f = state_work.f.view().force();
3313 for (index aid = cr->nodeid; aid < ssize(atom_index); aid += nnodes)
3315 size_t atom = atom_index[aid];
3316 for (size_t d = 0; d < DIM; d++)
3319 int force_flags = GMX_FORCE_STATECHANGED | GMX_FORCE_ALLFORCES;
3322 x_min = state_work_x[atom][d];
3324 for (unsigned int dx = 0; (dx < 2); dx++)
3328 state_work_x[atom][d] = x_min - der_range;
3332 state_work_x[atom][d] = x_min + der_range;
3335 /* Make evaluate_energy do a single node force calculation */
3339 /* Now is the time to relax the shells */
3340 relax_shell_flexcon(fplog,
3343 mdrunOptions.verbose,
3354 state_work.s.natoms,
3355 state_work.s.x.arrayRefWithPadding(),
3356 state_work.s.v.arrayRefWithPadding(),
3358 state_work.s.lambda,
3360 &state_work.f.view(),
3371 DDBalanceRegionHandler(nullptr));
3377 energyEvaluator.run(&state_work, mu_tot, vir, pres, aid * 2 + dx, FALSE, step);
3380 cr->nnodes = nnodes;
3384 std::copy(state_work_f.begin(), state_work_f.begin() + atom_index.size(), fneg.begin());
3388 /* x is restored to original */
3389 state_work_x[atom][d] = x_min;
3391 for (size_t j = 0; j < atom_index.size(); j++)
3393 for (size_t k = 0; (k < DIM); k++)
3395 dfdx[j][k] = -(state_work_f[atom_index[j]][k] - fneg[j][k]) / (2 * der_range);
3402 # define mpi_type GMX_MPI_REAL
3403 MPI_Send(dfdx[0], atom_index.size() * DIM, mpi_type, MASTER(cr), cr->nodeid, cr->mpi_comm_mygroup);
3408 for (index node = 0; (node < nnodes && aid + node < ssize(atom_index)); node++)
3414 MPI_Recv(dfdx[0], atom_index.size() * DIM, mpi_type, node, node, cr->mpi_comm_mygroup, &stat);
3419 row = (aid + node) * DIM + d;
3421 for (size_t j = 0; j < atom_index.size(); j++)
3423 for (size_t k = 0; k < DIM; k++)
3429 if (col >= row && dfdx[j][k] != 0.0)
3431 gmx_sparsematrix_increment_value(sparse_matrix, row, col, dfdx[j][k]);
3436 full_matrix[row * sz + col] = dfdx[j][k];
3443 if (mdrunOptions.verbose && fplog)
3448 /* write progress */
3449 if (bIsMaster && mdrunOptions.verbose)
3452 "\rFinished step %d out of %td",
3453 std::min<int>(atom + nnodes, atom_index.size()),
3461 fprintf(stderr, "\n\nWriting Hessian...\n");
3462 gmx_mtxio_write(ftp2fn(efMTX, nfile, fnm), sz, sz, full_matrix, sparse_matrix);
3465 finish_em(cr, outf, walltime_accounting, wcycle);
3467 walltime_accounting_set_nsteps_done(walltime_accounting, atom_index.size() * 2);