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48 #include "gromacs/domdec/domdec_struct.h"
49 #include "gromacs/fileio/confio.h"
50 #include "gromacs/gmxlib/network.h"
51 #include "gromacs/gmxlib/nrnb.h"
52 #include "gromacs/listed_forces/disre.h"
53 #include "gromacs/listed_forces/orires.h"
54 #include "gromacs/math/functions.h"
55 #include "gromacs/math/invertmatrix.h"
56 #include "gromacs/math/paddedvector.h"
57 #include "gromacs/math/units.h"
58 #include "gromacs/math/vec.h"
59 #include "gromacs/math/vecdump.h"
60 #include "gromacs/mdlib/boxdeformation.h"
61 #include "gromacs/mdlib/constr.h"
62 #include "gromacs/mdlib/gmx_omp_nthreads.h"
63 #include "gromacs/mdlib/mdatoms.h"
64 #include "gromacs/mdlib/stat.h"
65 #include "gromacs/mdlib/tgroup.h"
66 #include "gromacs/mdtypes/commrec.h"
67 #include "gromacs/mdtypes/fcdata.h"
68 #include "gromacs/mdtypes/group.h"
69 #include "gromacs/mdtypes/inputrec.h"
70 #include "gromacs/mdtypes/md_enums.h"
71 #include "gromacs/mdtypes/mdatom.h"
72 #include "gromacs/mdtypes/state.h"
73 #include "gromacs/pbcutil/boxutilities.h"
74 #include "gromacs/pbcutil/pbc.h"
75 #include "gromacs/pulling/pull.h"
76 #include "gromacs/random/tabulatednormaldistribution.h"
77 #include "gromacs/random/threefry.h"
78 #include "gromacs/simd/simd.h"
79 #include "gromacs/timing/wallcycle.h"
80 #include "gromacs/topology/atoms.h"
81 #include "gromacs/utility/exceptions.h"
82 #include "gromacs/utility/fatalerror.h"
83 #include "gromacs/utility/futil.h"
84 #include "gromacs/utility/gmxassert.h"
85 #include "gromacs/utility/gmxomp.h"
86 #include "gromacs/utility/smalloc.h"
88 using namespace gmx; // TODO: Remove when this file is moved into gmx namespace
103 std::vector<real> bd_rf;
105 std::vector<gmx_sd_const_t> sdc;
106 std::vector<gmx_sd_sigma_t> sdsig;
107 /* andersen temperature control stuff */
108 std::vector<bool> randomize_group;
109 std::vector<real> boltzfac;
111 explicit gmx_stochd_t(const t_inputrec& inputRecord);
114 //! pImpled implementation for Update
119 Impl(const t_inputrec& inputRecord, BoxDeformation* boxDeformation);
123 void update_coords(const t_inputrec& inputRecord,
126 bool havePartiallyFrozenAtoms,
127 gmx::ArrayRef<const ParticleType> ptype,
128 gmx::ArrayRef<const unsigned short> cFREEZE,
129 gmx::ArrayRef<const unsigned short> cTC,
130 gmx::ArrayRef<const real> invMass,
131 gmx::ArrayRef<rvec> invMassPerDim,
133 const gmx::ArrayRefWithPadding<const gmx::RVec>& f,
134 const t_fcdata& fcdata,
135 const gmx_ekindata_t* ekind,
139 bool haveConstraints);
141 void finish_update(const t_inputrec& inputRecord,
144 gmx_wallcycle_t wcycle,
145 bool haveConstraints);
147 void update_sd_second_half(const t_inputrec& inputRecord,
151 gmx::ArrayRef<const ParticleType> ptype,
152 gmx::ArrayRef<const unsigned short> cFREEZE,
153 gmx::ArrayRef<const unsigned short> cTC,
154 gmx::ArrayRef<const real> invMass,
158 gmx_wallcycle_t wcycle,
159 gmx::Constraints* constr,
163 void update_for_constraint_virial(const t_inputrec& inputRecord,
165 bool havePartiallyFrozenAtoms,
166 gmx::ArrayRef<real> invmass,
167 gmx::ArrayRef<rvec> invMassPerDim,
168 const t_state& state,
169 const gmx::ArrayRefWithPadding<const gmx::RVec>& f,
170 const gmx_ekindata_t& ekind);
172 void update_temperature_constants(const t_inputrec& inputRecord);
174 const std::vector<bool>& getAndersenRandomizeGroup() const { return sd_.randomize_group; }
176 const std::vector<real>& getBoltzmanFactor() const { return sd_.boltzfac; }
178 PaddedVector<RVec>* xp() { return &xp_; }
180 BoxDeformation* deform() const { return deform_; }
183 //! stochastic dynamics struct
185 //! xprime for constraint algorithms
186 PaddedVector<RVec> xp_;
187 //! Box deformation handler (or nullptr if inactive).
188 BoxDeformation* deform_ = nullptr;
191 Update::Update(const t_inputrec& inputRecord, BoxDeformation* boxDeformation) :
192 impl_(new Impl(inputRecord, boxDeformation)){};
196 const std::vector<bool>& Update::getAndersenRandomizeGroup() const
198 return impl_->getAndersenRandomizeGroup();
201 const std::vector<real>& Update::getBoltzmanFactor() const
203 return impl_->getBoltzmanFactor();
206 PaddedVector<RVec>* Update::xp()
211 BoxDeformation* Update::deform() const
213 return impl_->deform();
216 void Update::update_coords(const t_inputrec& inputRecord,
220 const gmx::ArrayRefWithPadding<const gmx::RVec>& f,
221 const t_fcdata& fcdata,
222 const gmx_ekindata_t* ekind,
226 const bool haveConstraints)
228 return impl_->update_coords(inputRecord,
231 md->havePartiallyFrozenAtoms,
232 gmx::arrayRefFromArray(md->ptype, md->nr),
233 md->cFREEZE ? gmx::arrayRefFromArray(md->cFREEZE, md->nr)
234 : gmx::ArrayRef<const unsigned short>(),
235 md->cTC ? gmx::arrayRefFromArray(md->cTC, md->nr)
236 : gmx::ArrayRef<const unsigned short>(),
237 gmx::arrayRefFromArray(md->invmass, md->nr),
238 gmx::arrayRefFromArray(md->invMassPerDim, md->nr),
249 void Update::finish_update(const t_inputrec& inputRecord,
252 gmx_wallcycle_t wcycle,
253 const bool haveConstraints)
255 return impl_->finish_update(inputRecord, md, state, wcycle, haveConstraints);
258 void Update::update_sd_second_half(const t_inputrec& inputRecord,
265 gmx_wallcycle_t wcycle,
266 gmx::Constraints* constr,
270 return impl_->update_sd_second_half(inputRecord,
274 gmx::arrayRefFromArray(md->ptype, md->nr),
275 md->cFREEZE ? gmx::arrayRefFromArray(md->cFREEZE, md->nr)
276 : gmx::ArrayRef<const unsigned short>(),
277 md->cTC ? gmx::arrayRefFromArray(md->cTC, md->nr)
278 : gmx::ArrayRef<const unsigned short>(),
279 gmx::arrayRefFromArray(md->invmass, md->nr),
289 void Update::update_for_constraint_virial(const t_inputrec& inputRecord,
291 const t_state& state,
292 const gmx::ArrayRefWithPadding<const gmx::RVec>& f,
293 const gmx_ekindata_t& ekind)
295 return impl_->update_for_constraint_virial(inputRecord,
297 md.havePartiallyFrozenAtoms,
298 gmx::arrayRefFromArray(md.invmass, md.nr),
299 gmx::arrayRefFromArray(md.invMassPerDim, md.nr),
305 void Update::update_temperature_constants(const t_inputrec& inputRecord)
307 return impl_->update_temperature_constants(inputRecord);
310 /*! \brief Sets whether we store the updated velocities */
311 enum class StoreUpdatedVelocities
313 yes, //!< Store the updated velocities
314 no //!< Do not store the updated velocities
317 /*! \brief Sets the number of different temperature coupling values */
318 enum class NumTempScaleValues
320 single, //!< Single T-scaling value (either one group or all values =1)
321 multiple //!< Multiple T-scaling values, need to use T-group indices
324 /*! \brief Sets if to apply no or diagonal Parrinello-Rahman pressure scaling
326 * Note that this enum is only used in updateMDLeapfrogSimple(), which does
327 * not handle fully anistropic Parrinello-Rahman scaling, so we only have
328 * options \p no and \p diagonal here and no anistropic option.
330 enum class ApplyParrinelloRahmanVScaling
332 no, //!< Do not apply velocity scaling (not a PR-coupling run or step)
333 diagonal //!< Apply velocity scaling using a diagonal matrix
336 /*! \brief Integrate using leap-frog with T-scaling and optionally diagonal Parrinello-Rahman p-coupling
338 * \tparam storeUpdatedVelocities Tells whether we should store the updated velocities
339 * \tparam numTempScaleValues The number of different T-couple values
340 * \tparam applyPRVScaling Apply Parrinello-Rahman velocity scaling
341 * \param[in] start Index of first atom to update
342 * \param[in] nrend Last atom to update: \p nrend - 1
343 * \param[in] dt The time step
344 * \param[in] dtPressureCouple Time step for pressure coupling
345 * \param[in] invMassPerDim 1/mass per atom and dimension
346 * \param[in] tcstat Temperature coupling information
347 * \param[in] cTC T-coupling group index per atom
348 * \param[in] pRVScaleMatrixDiagonal Parrinello-Rahman v-scale matrix diagonal
349 * \param[in] x Input coordinates
350 * \param[out] xprime Updated coordinates
351 * \param[inout] v Velocities, type either rvec* or const rvec*
352 * \param[in] f Forces
354 * We expect this template to get good SIMD acceleration by most compilers,
355 * unlike the more complex general template.
356 * Note that we might get even better SIMD acceleration when we introduce
357 * aligned (and padded) memory, possibly with some hints for the compilers.
359 template<StoreUpdatedVelocities storeUpdatedVelocities, NumTempScaleValues numTempScaleValues, ApplyParrinelloRahmanVScaling applyPRVScaling, typename VelocityType>
360 static std::enable_if_t<std::is_same<VelocityType, rvec>::value || std::is_same<VelocityType, const rvec>::value, void>
361 updateMDLeapfrogSimple(int start,
364 real dtPressureCouple,
365 gmx::ArrayRef<const rvec> invMassPerDim,
366 gmx::ArrayRef<const t_grp_tcstat> tcstat,
367 gmx::ArrayRef<const unsigned short> cTC,
368 const rvec pRVScaleMatrixDiagonal,
369 const rvec* gmx_restrict x,
370 rvec* gmx_restrict xprime,
371 VelocityType* gmx_restrict v,
372 const rvec* gmx_restrict f)
376 if (numTempScaleValues == NumTempScaleValues::single)
378 lambdaGroup = tcstat[0].lambda;
381 for (int a = start; a < nrend; a++)
383 if (numTempScaleValues == NumTempScaleValues::multiple)
385 lambdaGroup = tcstat[cTC[a]].lambda;
388 for (int d = 0; d < DIM; d++)
390 /* Note that using rvec invMassPerDim results in more efficient
391 * SIMD code, but this increases the cache pressure.
392 * For large systems with PME on the CPU this slows down the
393 * (then already slow) update by 20%. If all data remains in cache,
394 * using rvec is much faster.
396 real vNew = lambdaGroup * v[a][d] + f[a][d] * invMassPerDim[a][d] * dt;
398 if (applyPRVScaling == ApplyParrinelloRahmanVScaling::diagonal)
400 vNew -= dtPressureCouple * pRVScaleMatrixDiagonal[d] * v[a][d];
402 // TODO: Remove NOLINTs once clang-tidy is updated to v11, it should be able to handle constexpr.
403 if constexpr (storeUpdatedVelocities == StoreUpdatedVelocities::yes) // NOLINT // NOLINTNEXTLINE
407 xprime[a][d] = x[a][d] + vNew * dt; // NOLINT(readability-misleading-indentation)
412 #if GMX_SIMD && GMX_SIMD_HAVE_REAL
413 # define GMX_HAVE_SIMD_UPDATE 1
415 # define GMX_HAVE_SIMD_UPDATE 0
418 #if GMX_HAVE_SIMD_UPDATE
420 /*! \brief Load (aligned) the contents of GMX_SIMD_REAL_WIDTH rvec elements sequentially into 3 SIMD registers
422 * The loaded output is:
423 * \p r0: { r[index][XX], r[index][YY], ... }
425 * \p r2: { ..., r[index+GMX_SIMD_REAL_WIDTH-1][YY], r[index+GMX_SIMD_REAL_WIDTH-1][ZZ] }
427 * \param[in] r Real to an rvec array, has to be aligned to SIMD register width
428 * \param[in] index Index of the first rvec triplet of reals to load
429 * \param[out] r0 Pointer to first SIMD register
430 * \param[out] r1 Pointer to second SIMD register
431 * \param[out] r2 Pointer to third SIMD register
433 static inline void simdLoadRvecs(const rvec* r, int index, SimdReal* r0, SimdReal* r1, SimdReal* r2)
435 const real* realPtr = r[index];
437 GMX_ASSERT(isSimdAligned(realPtr), "Pointer should be SIMD aligned");
439 *r0 = simdLoad(realPtr + 0 * GMX_SIMD_REAL_WIDTH);
440 *r1 = simdLoad(realPtr + 1 * GMX_SIMD_REAL_WIDTH);
441 *r2 = simdLoad(realPtr + 2 * GMX_SIMD_REAL_WIDTH);
444 /*! \brief Store (aligned) 3 SIMD registers sequentially to GMX_SIMD_REAL_WIDTH rvec elements
446 * The stored output is:
447 * \p r[index] = { { r0[0], r0[1], ... }
449 * \p r[index+GMX_SIMD_REAL_WIDTH-1] = { ... , r2[GMX_SIMD_REAL_WIDTH-2], r2[GMX_SIMD_REAL_WIDTH-1] }
451 * \param[out] r Pointer to an rvec array, has to be aligned to SIMD register width
452 * \param[in] index Index of the first rvec triplet of reals to store to
453 * \param[in] r0 First SIMD register
454 * \param[in] r1 Second SIMD register
455 * \param[in] r2 Third SIMD register
457 static inline void simdStoreRvecs(rvec* r, int index, SimdReal r0, SimdReal r1, SimdReal r2)
459 real* realPtr = r[index];
461 GMX_ASSERT(isSimdAligned(realPtr), "Pointer should be SIMD aligned");
463 store(realPtr + 0 * GMX_SIMD_REAL_WIDTH, r0);
464 store(realPtr + 1 * GMX_SIMD_REAL_WIDTH, r1);
465 store(realPtr + 2 * GMX_SIMD_REAL_WIDTH, r2);
468 /*! \brief Integrate using leap-frog with single group T-scaling and SIMD
470 * \tparam storeUpdatedVelocities Tells whether we should store the updated velocities
471 * \param[in] start Index of first atom to update
472 * \param[in] nrend Last atom to update: \p nrend - 1
473 * \param[in] dt The time step
474 * \param[in] invMass 1/mass per atom
475 * \param[in] tcstat Temperature coupling information
476 * \param[in] x Input coordinates
477 * \param[out] xprime Updated coordinates
478 * \param[inout] v Velocities, type either rvec* or const rvec*
479 * \param[in] f Forces
481 template<StoreUpdatedVelocities storeUpdatedVelocities, typename VelocityType>
482 static std::enable_if_t<std::is_same<VelocityType, rvec>::value || std::is_same<VelocityType, const rvec>::value, void>
483 updateMDLeapfrogSimpleSimd(int start,
486 gmx::ArrayRef<const real> invMass,
487 gmx::ArrayRef<const t_grp_tcstat> tcstat,
488 const rvec* gmx_restrict x,
489 rvec* gmx_restrict xprime,
490 VelocityType* gmx_restrict v,
491 const rvec* gmx_restrict f)
493 SimdReal timestep(dt);
494 SimdReal lambdaSystem(tcstat[0].lambda);
496 /* We declare variables here, since code is often slower when declaring them inside the loop */
498 /* Note: We should implement a proper PaddedVector, so we don't need this check */
499 GMX_ASSERT(isSimdAligned(invMass.data()), "invMass should be aligned");
501 for (int a = start; a < nrend; a += GMX_SIMD_REAL_WIDTH)
503 SimdReal invMass0, invMass1, invMass2;
504 expandScalarsToTriplets(simdLoad(invMass.data() + a), &invMass0, &invMass1, &invMass2);
508 simdLoadRvecs(v, a, &v0, &v1, &v2);
509 simdLoadRvecs(f, a, &f0, &f1, &f2);
511 v0 = fma(f0 * invMass0, timestep, lambdaSystem * v0);
512 v1 = fma(f1 * invMass1, timestep, lambdaSystem * v1);
513 v2 = fma(f2 * invMass2, timestep, lambdaSystem * v2);
515 // TODO: Remove NOLINTs once clang-tidy is updated to v11, it should be able to handle constexpr.
516 if constexpr (storeUpdatedVelocities == StoreUpdatedVelocities::yes) // NOLINT // NOLINTNEXTLINE
518 simdStoreRvecs(v, a, v0, v1, v2);
521 SimdReal x0, x1, x2; // NOLINT(readability-misleading-indentation)
522 simdLoadRvecs(x, a, &x0, &x1, &x2);
524 SimdReal xprime0 = fma(v0, timestep, x0);
525 SimdReal xprime1 = fma(v1, timestep, x1);
526 SimdReal xprime2 = fma(v2, timestep, x2);
528 simdStoreRvecs(xprime, a, xprime0, xprime1, xprime2);
532 #endif // GMX_HAVE_SIMD_UPDATE
534 /*! \brief Sets the NEMD acceleration type */
535 enum class AccelerationType
541 /*! \brief Integrate using leap-frog with support for everything.
543 * \tparam accelerationType Type of NEMD acceleration.
544 * \param[in] start Index of first atom to update.
545 * \param[in] nrend Last atom to update: \p nrend - 1.
546 * \param[in] doNoseHoover If to apply Nose-Hoover T-coupling.
547 * \param[in] dt The time step.
548 * \param[in] dtPressureCouple Time step for pressure coupling, is 0 when no pressure
549 * coupling should be applied at this step.
550 * \param[in] cTC Temperature coupling group indices
551 * \param[in] invMassPerDim Inverse mass per dimension
552 * \param[in] ekind Kinetic energy data.
553 * \param[in] box The box dimensions.
554 * \param[in] x Input coordinates.
555 * \param[out] xprime Updated coordinates.
556 * \param[inout] v Velocities.
557 * \param[in] f Forces.
558 * \param[in] nh_vxi Nose-Hoover velocity scaling factors.
559 * \param[in] nsttcouple Frequency of the temperature coupling steps.
560 * \param[in] M Parrinello-Rahman scaling matrix.
562 template<AccelerationType accelerationType>
563 static void updateMDLeapfrogGeneral(int start,
567 real dtPressureCouple,
568 gmx::ArrayRef<const unsigned short> cTC,
569 gmx::ArrayRef<const rvec> invMassPerDim,
570 const gmx_ekindata_t* ekind,
572 const rvec* gmx_restrict x,
573 rvec* gmx_restrict xprime,
574 rvec* gmx_restrict v,
575 const rvec* gmx_restrict f,
576 const double* gmx_restrict nh_vxi,
577 const int nsttcouple,
580 /* This is a version of the leap-frog integrator that supports
581 * all combinations of T-coupling, P-coupling and NEMD.
582 * Nose-Hoover uses the reversible leap-frog integrator from
583 * Holian et al. Phys Rev E 52(3) : 2338, 1995
586 gmx::ArrayRef<const t_grp_tcstat> tcstat = ekind->tcstat;
588 /* Initialize group values, changed later when multiple groups are used */
591 real omega_Z = 2 * static_cast<real>(M_PI) / box[ZZ][ZZ];
593 for (int n = start; n < nrend; n++)
599 real lg = tcstat[gt].lambda;
602 real cosineZ, vCosine;
603 switch (accelerationType)
605 case AccelerationType::none: copy_rvec(v[n], vRel); break;
606 case AccelerationType::cosine:
607 cosineZ = std::cos(x[n][ZZ] * omega_Z);
608 vCosine = cosineZ * ekind->cosacc.vcos;
609 /* Avoid scaling the cosine profile velocity */
610 copy_rvec(v[n], vRel);
618 /* Here we account for multiple time stepping, by increasing
619 * the Nose-Hoover correction by nsttcouple
620 * TODO: This can be pre-computed.
622 factorNH = 0.5 * nsttcouple * dt * nh_vxi[gt];
625 for (int d = 0; d < DIM; d++)
627 real vNew = (lg * vRel[d]
628 + (f[n][d] * invMassPerDim[n][d] * dt - factorNH * vRel[d]
629 - dtPressureCouple * iprod(M[d], vRel)))
631 switch (accelerationType)
633 case AccelerationType::none: break;
634 case AccelerationType::cosine:
637 /* Add back the mean velocity and apply acceleration */
638 vNew += vCosine + cosineZ * ekind->cosacc.cos_accel * dt;
643 xprime[n][d] = x[n][d] + vNew * dt;
648 /*! \brief Handles the Leap-frog MD x and v integration */
649 static void do_update_md(int start,
653 const rvec* gmx_restrict x,
654 rvec* gmx_restrict xprime,
655 rvec* gmx_restrict v,
656 const rvec* gmx_restrict f,
657 const TemperatureCoupling etc,
658 const PressureCoupling epc,
659 const int nsttcouple,
660 const int nstpcouple,
661 gmx::ArrayRef<const unsigned short> cTC,
662 gmx::ArrayRef<const real> gmx_unused invmass,
663 gmx::ArrayRef<const rvec> invMassPerDim,
664 const gmx_ekindata_t* ekind,
666 const double* gmx_restrict nh_vxi,
668 bool gmx_unused havePartiallyFrozenAtoms)
670 GMX_ASSERT(nrend == start || xprime != x,
671 "For SIMD optimization certain compilers need to have xprime != x");
673 /* Note: Berendsen pressure scaling is handled after do_update_md() */
675 (etc != TemperatureCoupling::No && do_per_step(step + nsttcouple - 1, nsttcouple));
676 bool doNoseHoover = (etc == TemperatureCoupling::NoseHoover && doTempCouple);
677 bool doParrinelloRahman = (epc == PressureCoupling::ParrinelloRahman
678 && do_per_step(step + nstpcouple - 1, nstpcouple));
679 bool doPROffDiagonal = (doParrinelloRahman && (M[YY][XX] != 0 || M[ZZ][XX] != 0 || M[ZZ][YY] != 0));
681 real dtPressureCouple = (doParrinelloRahman ? nstpcouple * dt : 0);
683 /* NEMD cosine acceleration is applied in updateMDLeapFrogGeneral */
684 bool doAcceleration = (ekind->cosacc.cos_accel != 0);
686 if (doNoseHoover || doPROffDiagonal || doAcceleration)
689 if (!doParrinelloRahman)
691 /* We should not apply PR scaling at this step */
701 updateMDLeapfrogGeneral<AccelerationType::none>(start,
720 updateMDLeapfrogGeneral<AccelerationType::cosine>(start,
740 /* We determine if we have a single T-coupling lambda value for all
741 * atoms. That allows for better SIMD acceleration in the template.
742 * If we do not do temperature coupling (in the run or this step),
743 * all scaling values are 1, so we effectively have a single value.
745 bool haveSingleTempScaleValue = (!doTempCouple || ekind->ngtc == 1);
747 /* Extract some pointers needed by all cases */
748 gmx::ArrayRef<const t_grp_tcstat> tcstat = ekind->tcstat;
750 if (doParrinelloRahman)
752 GMX_ASSERT(!doPROffDiagonal,
753 "updateMDLeapfrogSimple only support diagonal Parrinello-Rahman scaling "
757 for (int d = 0; d < DIM; d++)
762 if (haveSingleTempScaleValue)
764 updateMDLeapfrogSimple<StoreUpdatedVelocities::yes, NumTempScaleValues::single, ApplyParrinelloRahmanVScaling::diagonal>(
765 start, nrend, dt, dtPressureCouple, invMassPerDim, tcstat, cTC, diagM, x, xprime, v, f);
769 updateMDLeapfrogSimple<StoreUpdatedVelocities::yes, NumTempScaleValues::multiple, ApplyParrinelloRahmanVScaling::diagonal>(
770 start, nrend, dt, dtPressureCouple, invMassPerDim, tcstat, cTC, diagM, x, xprime, v, f);
775 if (haveSingleTempScaleValue)
777 /* Note that modern compilers are pretty good at vectorizing
778 * updateMDLeapfrogSimple(). But the SIMD version will still
779 * be faster because invMass lowers the cache pressure
780 * compared to invMassPerDim.
782 #if GMX_HAVE_SIMD_UPDATE
783 /* Check if we can use invmass instead of invMassPerDim */
784 if (!havePartiallyFrozenAtoms)
786 updateMDLeapfrogSimpleSimd<StoreUpdatedVelocities::yes>(
787 start, nrend, dt, invmass, tcstat, x, xprime, v, f);
792 updateMDLeapfrogSimple<StoreUpdatedVelocities::yes, NumTempScaleValues::single, ApplyParrinelloRahmanVScaling::no>(
793 start, nrend, dt, dtPressureCouple, invMassPerDim, tcstat, cTC, nullptr, x, xprime, v, f);
798 updateMDLeapfrogSimple<StoreUpdatedVelocities::yes, NumTempScaleValues::multiple, ApplyParrinelloRahmanVScaling::no>(
799 start, nrend, dt, dtPressureCouple, invMassPerDim, tcstat, cTC, nullptr, x, xprime, v, f);
804 /*! \brief Handles the Leap-frog MD x and v integration */
805 static void doUpdateMDDoNotUpdateVelocities(int start,
808 const rvec* gmx_restrict x,
809 rvec* gmx_restrict xprime,
810 const rvec* gmx_restrict v,
811 const rvec* gmx_restrict f,
812 bool gmx_unused havePartiallyFrozenAtoms,
813 gmx::ArrayRef<real> gmx_unused invmass,
814 gmx::ArrayRef<rvec> invMassPerDim,
815 const gmx_ekindata_t& ekind)
817 GMX_ASSERT(nrend == start || xprime != x,
818 "For SIMD optimization certain compilers need to have xprime != x");
820 gmx::ArrayRef<const t_grp_tcstat> tcstat = ekind.tcstat;
822 /* Check if we can use invmass instead of invMassPerDim */
823 #if GMX_HAVE_SIMD_UPDATE
824 if (!havePartiallyFrozenAtoms)
826 updateMDLeapfrogSimpleSimd<StoreUpdatedVelocities::no>(
827 start, nrend, dt, invmass, tcstat, x, xprime, v, f);
832 updateMDLeapfrogSimple<StoreUpdatedVelocities::no, NumTempScaleValues::single, ApplyParrinelloRahmanVScaling::no>(
833 start, nrend, dt, dt, invMassPerDim, tcstat, gmx::ArrayRef<const unsigned short>(), nullptr, x, xprime, v, f);
837 static void do_update_vv_vel(int start,
840 gmx::ArrayRef<const ivec> nFreeze,
841 gmx::ArrayRef<const real> invmass,
842 gmx::ArrayRef<const ParticleType> ptype,
843 gmx::ArrayRef<const unsigned short> cFREEZE,
856 g = 0.25 * dt * veta * alpha;
858 mv2 = gmx::series_sinhx(g);
865 for (n = start; n < nrend; n++)
867 real w_dt = invmass[n] * dt;
868 if (!cFREEZE.empty())
873 for (d = 0; d < DIM; d++)
875 if ((ptype[n] != ParticleType::Shell) && !nFreeze[gf][d])
877 v[n][d] = mv1 * (mv1 * v[n][d] + 0.5 * (w_dt * mv2 * f[n][d]));
885 } /* do_update_vv_vel */
887 static void do_update_vv_pos(int start,
890 gmx::ArrayRef<const ivec> nFreeze,
891 gmx::ArrayRef<const ParticleType> ptype,
892 gmx::ArrayRef<const unsigned short> cFREEZE,
903 /* Would it make more sense if Parrinello-Rahman was put here? */
908 mr2 = gmx::series_sinhx(g);
916 for (n = start; n < nrend; n++)
919 if (!cFREEZE.empty())
924 for (d = 0; d < DIM; d++)
926 if ((ptype[n] != ParticleType::Shell) && !nFreeze[gf][d])
928 xprime[n][d] = mr1 * (mr1 * x[n][d] + mr2 * dt * v[n][d]);
932 xprime[n][d] = x[n][d];
936 } /* do_update_vv_pos */
938 gmx_stochd_t::gmx_stochd_t(const t_inputrec& inputRecord)
940 const t_grpopts* opts = &inputRecord.opts;
941 const int ngtc = opts->ngtc;
943 if (inputRecord.eI == IntegrationAlgorithm::BD)
947 else if (EI_SD(inputRecord.eI))
952 for (int gt = 0; gt < ngtc; gt++)
954 if (opts->tau_t[gt] > 0)
956 sdc[gt].em = std::exp(-inputRecord.delta_t / opts->tau_t[gt]);
960 /* No friction and noise on this group */
965 else if (ETC_ANDERSEN(inputRecord.etc))
967 randomize_group.resize(ngtc);
968 boltzfac.resize(ngtc);
970 /* for now, assume that all groups, if randomized, are randomized at the same rate, i.e. tau_t is the same. */
971 /* since constraint groups don't necessarily match up with temperature groups! This is checked in readir.c */
973 for (int gt = 0; gt < ngtc; gt++)
975 real reft = std::max<real>(0, opts->ref_t[gt]);
976 if ((opts->tau_t[gt] > 0)
977 && (reft > 0)) /* tau_t or ref_t = 0 means that no randomization is done */
979 randomize_group[gt] = true;
980 boltzfac[gt] = gmx::c_boltz * opts->ref_t[gt];
984 randomize_group[gt] = false;
990 void Update::Impl::update_temperature_constants(const t_inputrec& inputRecord)
992 if (inputRecord.eI == IntegrationAlgorithm::BD)
994 if (inputRecord.bd_fric != 0)
996 for (int gt = 0; gt < inputRecord.opts.ngtc; gt++)
998 sd_.bd_rf[gt] = std::sqrt(2.0 * gmx::c_boltz * inputRecord.opts.ref_t[gt]
999 / (inputRecord.bd_fric * inputRecord.delta_t));
1004 for (int gt = 0; gt < inputRecord.opts.ngtc; gt++)
1006 sd_.bd_rf[gt] = std::sqrt(2.0 * gmx::c_boltz * inputRecord.opts.ref_t[gt]);
1010 if (inputRecord.eI == IntegrationAlgorithm::SD1)
1012 for (int gt = 0; gt < inputRecord.opts.ngtc; gt++)
1014 real kT = gmx::c_boltz * inputRecord.opts.ref_t[gt];
1015 /* The mass is accounted for later, since this differs per atom */
1016 sd_.sdsig[gt].V = std::sqrt(kT * (1 - sd_.sdc[gt].em * sd_.sdc[gt].em));
1021 Update::Impl::Impl(const t_inputrec& inputRecord, BoxDeformation* boxDeformation) :
1023 deform_(boxDeformation)
1025 update_temperature_constants(inputRecord);
1026 xp_.resizeWithPadding(0);
1029 void Update::setNumAtoms(int numAtoms)
1032 impl_->xp()->resizeWithPadding(numAtoms);
1035 /*! \brief Sets the SD update type */
1036 enum class SDUpdate : int
1039 FrictionAndNoiseOnly,
1043 /*! \brief SD integrator update
1045 * Two phases are required in the general case of a constrained
1046 * update, the first phase from the contribution of forces, before
1047 * applying constraints, and then a second phase applying the friction
1048 * and noise, and then further constraining. For details, see
1051 * Without constraints, the two phases can be combined, for
1054 * Thus three instantiations of this templated function will be made,
1055 * two with only one contribution, and one with both contributions. */
1056 template<SDUpdate updateType>
1057 static void doSDUpdateGeneral(const gmx_stochd_t& sd,
1061 gmx::ArrayRef<const ivec> nFreeze,
1062 gmx::ArrayRef<const real> invmass,
1063 gmx::ArrayRef<const ParticleType> ptype,
1064 gmx::ArrayRef<const unsigned short> cFREEZE,
1065 gmx::ArrayRef<const unsigned short> cTC,
1072 const int* gatindex)
1074 // cTC and cFREEZE can be nullptr any time, but various
1075 // instantiations do not make sense with particular pointer
1077 if (updateType == SDUpdate::ForcesOnly)
1079 GMX_ASSERT(f != nullptr, "SD update with only forces requires forces");
1080 GMX_ASSERT(cTC.empty(), "SD update with only forces cannot handle temperature groups");
1082 if (updateType == SDUpdate::FrictionAndNoiseOnly)
1084 GMX_ASSERT(f == nullptr, "SD update with only noise cannot handle forces");
1086 if (updateType == SDUpdate::Combined)
1088 GMX_ASSERT(f != nullptr, "SD update with forces and noise requires forces");
1091 // Even 0 bits internal counter gives 2x64 ints (more than enough for three table lookups)
1092 gmx::ThreeFry2x64<0> rng(seed, gmx::RandomDomain::UpdateCoordinates);
1093 gmx::TabulatedNormalDistribution<real, 14> dist;
1095 for (int n = start; n < nrend; n++)
1097 int globalAtomIndex = gatindex ? gatindex[n] : n;
1098 rng.restart(step, globalAtomIndex);
1101 real inverseMass = invmass[n];
1102 real invsqrtMass = std::sqrt(inverseMass);
1104 int freezeGroup = !cFREEZE.empty() ? cFREEZE[n] : 0;
1105 int temperatureGroup = !cTC.empty() ? cTC[n] : 0;
1107 for (int d = 0; d < DIM; d++)
1109 if ((ptype[n] != ParticleType::Shell) && !nFreeze[freezeGroup][d])
1111 if (updateType == SDUpdate::ForcesOnly)
1113 real vn = v[n][d] + inverseMass * f[n][d] * dt;
1115 // Simple position update.
1116 xprime[n][d] = x[n][d] + v[n][d] * dt;
1118 else if (updateType == SDUpdate::FrictionAndNoiseOnly)
1121 v[n][d] = (vn * sd.sdc[temperatureGroup].em
1122 + invsqrtMass * sd.sdsig[temperatureGroup].V * dist(rng));
1123 // The previous phase already updated the
1124 // positions with a full v*dt term that must
1125 // now be half removed.
1126 xprime[n][d] = xprime[n][d] + 0.5 * (v[n][d] - vn) * dt;
1130 real vn = v[n][d] + inverseMass * f[n][d] * dt;
1131 v[n][d] = (vn * sd.sdc[temperatureGroup].em
1132 + invsqrtMass * sd.sdsig[temperatureGroup].V * dist(rng));
1133 // Here we include half of the friction+noise
1134 // update of v into the position update.
1135 xprime[n][d] = x[n][d] + 0.5 * (vn + v[n][d]) * dt;
1140 // When using constraints, the update is split into
1141 // two phases, but we only need to zero the update of
1142 // virtual, shell or frozen particles in at most one
1144 if (updateType != SDUpdate::FrictionAndNoiseOnly)
1147 xprime[n][d] = x[n][d];
1154 static void do_update_sd(int start,
1158 const rvec* gmx_restrict x,
1159 rvec* gmx_restrict xprime,
1160 rvec* gmx_restrict v,
1161 const rvec* gmx_restrict f,
1162 gmx::ArrayRef<const ivec> nFreeze,
1163 gmx::ArrayRef<const real> invmass,
1164 gmx::ArrayRef<const ParticleType> ptype,
1165 gmx::ArrayRef<const unsigned short> cFREEZE,
1166 gmx::ArrayRef<const unsigned short> cTC,
1168 const t_commrec* cr,
1169 const gmx_stochd_t& sd,
1170 bool haveConstraints)
1172 if (haveConstraints)
1174 // With constraints, the SD update is done in 2 parts
1175 doSDUpdateGeneral<SDUpdate::ForcesOnly>(sd,
1183 gmx::ArrayRef<const unsigned short>(),
1194 doSDUpdateGeneral<SDUpdate::Combined>(sd,
1209 DOMAINDECOMP(cr) ? cr->dd->globalAtomIndices.data() : nullptr);
1213 static void do_update_bd(int start,
1217 const rvec* gmx_restrict x,
1218 rvec* gmx_restrict xprime,
1219 rvec* gmx_restrict v,
1220 const rvec* gmx_restrict f,
1221 gmx::ArrayRef<const ivec> nFreeze,
1222 gmx::ArrayRef<const real> invmass,
1223 gmx::ArrayRef<const ParticleType> ptype,
1224 gmx::ArrayRef<const unsigned short> cFREEZE,
1225 gmx::ArrayRef<const unsigned short> cTC,
1226 real friction_coefficient,
1229 const int* gatindex)
1231 /* note -- these appear to be full step velocities . . . */
1236 // Use 1 bit of internal counters to give us 2*2 64-bits values per stream
1237 // Each 64-bit value is enough for 4 normal distribution table numbers.
1238 gmx::ThreeFry2x64<0> rng(seed, gmx::RandomDomain::UpdateCoordinates);
1239 gmx::TabulatedNormalDistribution<real, 14> dist;
1241 if (friction_coefficient != 0)
1243 invfr = 1.0 / friction_coefficient;
1246 for (n = start; (n < nrend); n++)
1248 int ng = gatindex ? gatindex[n] : n;
1250 rng.restart(step, ng);
1253 if (!cFREEZE.empty())
1261 for (d = 0; (d < DIM); d++)
1263 if ((ptype[n] != ParticleType::Shell) && !nFreeze[gf][d])
1265 if (friction_coefficient != 0)
1267 vn = invfr * f[n][d] + rf[gt] * dist(rng);
1271 /* NOTE: invmass = 2/(mass*friction_constant*dt) */
1272 vn = 0.5 * invmass[n] * f[n][d] * dt
1273 + std::sqrt(0.5 * invmass[n]) * rf[gt] * dist(rng);
1277 xprime[n][d] = x[n][d] + vn * dt;
1282 xprime[n][d] = x[n][d];
1288 extern void init_ekinstate(ekinstate_t* ekinstate, const t_inputrec* ir)
1290 ekinstate->ekin_n = ir->opts.ngtc;
1291 snew(ekinstate->ekinh, ekinstate->ekin_n);
1292 snew(ekinstate->ekinf, ekinstate->ekin_n);
1293 snew(ekinstate->ekinh_old, ekinstate->ekin_n);
1294 ekinstate->ekinscalef_nhc.resize(ekinstate->ekin_n);
1295 ekinstate->ekinscaleh_nhc.resize(ekinstate->ekin_n);
1296 ekinstate->vscale_nhc.resize(ekinstate->ekin_n);
1297 ekinstate->dekindl = 0;
1298 ekinstate->mvcos = 0;
1299 ekinstate->hasReadEkinState = false;
1302 void update_ekinstate(ekinstate_t* ekinstate, const gmx_ekindata_t* ekind)
1306 for (i = 0; i < ekinstate->ekin_n; i++)
1308 copy_mat(ekind->tcstat[i].ekinh, ekinstate->ekinh[i]);
1309 copy_mat(ekind->tcstat[i].ekinf, ekinstate->ekinf[i]);
1310 copy_mat(ekind->tcstat[i].ekinh_old, ekinstate->ekinh_old[i]);
1311 ekinstate->ekinscalef_nhc[i] = ekind->tcstat[i].ekinscalef_nhc;
1312 ekinstate->ekinscaleh_nhc[i] = ekind->tcstat[i].ekinscaleh_nhc;
1313 ekinstate->vscale_nhc[i] = ekind->tcstat[i].vscale_nhc;
1316 copy_mat(ekind->ekin, ekinstate->ekin_total);
1317 ekinstate->dekindl = ekind->dekindl;
1318 ekinstate->mvcos = ekind->cosacc.mvcos;
1321 void restore_ekinstate_from_state(const t_commrec* cr, gmx_ekindata_t* ekind, const ekinstate_t* ekinstate)
1327 for (i = 0; i < ekinstate->ekin_n; i++)
1329 copy_mat(ekinstate->ekinh[i], ekind->tcstat[i].ekinh);
1330 copy_mat(ekinstate->ekinf[i], ekind->tcstat[i].ekinf);
1331 copy_mat(ekinstate->ekinh_old[i], ekind->tcstat[i].ekinh_old);
1332 ekind->tcstat[i].ekinscalef_nhc = ekinstate->ekinscalef_nhc[i];
1333 ekind->tcstat[i].ekinscaleh_nhc = ekinstate->ekinscaleh_nhc[i];
1334 ekind->tcstat[i].vscale_nhc = ekinstate->vscale_nhc[i];
1337 copy_mat(ekinstate->ekin_total, ekind->ekin);
1339 ekind->dekindl = ekinstate->dekindl;
1340 ekind->cosacc.mvcos = ekinstate->mvcos;
1341 n = ekinstate->ekin_n;
1346 gmx_bcast(sizeof(n), &n, cr->mpi_comm_mygroup);
1347 for (i = 0; i < n; i++)
1349 gmx_bcast(DIM * DIM * sizeof(ekind->tcstat[i].ekinh[0][0]),
1350 ekind->tcstat[i].ekinh[0],
1351 cr->mpi_comm_mygroup);
1352 gmx_bcast(DIM * DIM * sizeof(ekind->tcstat[i].ekinf[0][0]),
1353 ekind->tcstat[i].ekinf[0],
1354 cr->mpi_comm_mygroup);
1355 gmx_bcast(DIM * DIM * sizeof(ekind->tcstat[i].ekinh_old[0][0]),
1356 ekind->tcstat[i].ekinh_old[0],
1357 cr->mpi_comm_mygroup);
1359 gmx_bcast(sizeof(ekind->tcstat[i].ekinscalef_nhc),
1360 &(ekind->tcstat[i].ekinscalef_nhc),
1361 cr->mpi_comm_mygroup);
1362 gmx_bcast(sizeof(ekind->tcstat[i].ekinscaleh_nhc),
1363 &(ekind->tcstat[i].ekinscaleh_nhc),
1364 cr->mpi_comm_mygroup);
1365 gmx_bcast(sizeof(ekind->tcstat[i].vscale_nhc), &(ekind->tcstat[i].vscale_nhc), cr->mpi_comm_mygroup);
1367 gmx_bcast(DIM * DIM * sizeof(ekind->ekin[0][0]), ekind->ekin[0], cr->mpi_comm_mygroup);
1369 gmx_bcast(sizeof(ekind->dekindl), &ekind->dekindl, cr->mpi_comm_mygroup);
1370 gmx_bcast(sizeof(ekind->cosacc.mvcos), &ekind->cosacc.mvcos, cr->mpi_comm_mygroup);
1374 void getThreadAtomRange(int numThreads, int threadIndex, int numAtoms, int* startAtom, int* endAtom)
1376 #if GMX_HAVE_SIMD_UPDATE
1377 constexpr int blockSize = GMX_SIMD_REAL_WIDTH;
1379 constexpr int blockSize = 1;
1381 int numBlocks = (numAtoms + blockSize - 1) / blockSize;
1383 *startAtom = ((numBlocks * threadIndex) / numThreads) * blockSize;
1384 *endAtom = ((numBlocks * (threadIndex + 1)) / numThreads) * blockSize;
1385 if (threadIndex == numThreads - 1)
1387 *endAtom = numAtoms;
1391 void Update::Impl::update_sd_second_half(const t_inputrec& inputRecord,
1395 gmx::ArrayRef<const ParticleType> ptype,
1396 gmx::ArrayRef<const unsigned short> cFREEZE,
1397 gmx::ArrayRef<const unsigned short> cTC,
1398 gmx::ArrayRef<const real> invMass,
1400 const t_commrec* cr,
1402 gmx_wallcycle_t wcycle,
1403 gmx::Constraints* constr,
1411 if (inputRecord.eI == IntegrationAlgorithm::SD1)
1414 /* Cast delta_t from double to real to make the integrators faster.
1415 * The only reason for having delta_t double is to get accurate values
1416 * for t=delta_t*step when step is larger than float precision.
1417 * For integration dt the accuracy of real suffices, since with
1418 * integral += dt*integrand the increment is nearly always (much) smaller
1419 * than the integral (and the integrand has real precision).
1421 real dt = inputRecord.delta_t;
1423 wallcycle_start(wcycle, ewcUPDATE);
1425 int nth = gmx_omp_nthreads_get(emntUpdate);
1427 #pragma omp parallel for num_threads(nth) schedule(static)
1428 for (int th = 0; th < nth; th++)
1432 int start_th, end_th;
1433 getThreadAtomRange(nth, th, homenr, &start_th, &end_th);
1435 doSDUpdateGeneral<SDUpdate::FrictionAndNoiseOnly>(
1440 gmx::arrayRefFromArray(inputRecord.opts.nFreeze, inputRecord.opts.ngfrz),
1445 state->x.rvec_array(),
1447 state->v.rvec_array(),
1450 inputRecord.ld_seed,
1451 DOMAINDECOMP(cr) ? cr->dd->globalAtomIndices.data() : nullptr);
1453 GMX_CATCH_ALL_AND_EXIT_WITH_FATAL_ERROR
1455 inc_nrnb(nrnb, eNR_UPDATE, homenr);
1456 wallcycle_stop(wcycle, ewcUPDATE);
1458 /* Constrain the coordinates upd->xp for half a time step */
1459 bool computeVirial = false;
1460 constr->apply(do_log,
1465 state->x.arrayRefWithPadding(),
1466 xp_.arrayRefWithPadding(),
1469 state->lambda[static_cast<int>(FreeEnergyPerturbationCouplingType::Bonded)],
1471 state->v.arrayRefWithPadding(),
1474 ConstraintVariable::Positions);
1478 void Update::Impl::finish_update(const t_inputrec& inputRecord,
1479 const t_mdatoms* md,
1481 gmx_wallcycle_t wcycle,
1482 const bool haveConstraints)
1484 /* NOTE: Currently we always integrate to a temporary buffer and
1485 * then copy the results back here.
1488 wallcycle_start_nocount(wcycle, ewcUPDATE);
1490 const int homenr = md->homenr;
1491 auto xp = makeConstArrayRef(xp_).subArray(0, homenr);
1492 auto x = makeArrayRef(state->x).subArray(0, homenr);
1494 if (md->havePartiallyFrozenAtoms && haveConstraints)
1496 /* We have atoms that are frozen along some, but not all dimensions,
1497 * then constraints will have moved them also along the frozen dimensions.
1498 * To freeze such degrees of freedom we do not copy them back here.
1500 const ivec* nFreeze = inputRecord.opts.nFreeze;
1502 for (int i = 0; i < homenr; i++)
1504 const int g = md->cFREEZE[i];
1506 for (int d = 0; d < DIM; d++)
1508 if (nFreeze[g][d] == 0)
1517 /* We have no frozen atoms or fully frozen atoms which have not
1518 * been moved by the update, so we can simply copy all coordinates.
1520 int gmx_unused nth = gmx_omp_nthreads_get(emntUpdate);
1521 #pragma omp parallel for num_threads(nth) schedule(static)
1522 for (int i = 0; i < homenr; i++)
1524 // Trivial statement, does not throw
1529 wallcycle_stop(wcycle, ewcUPDATE);
1532 void Update::Impl::update_coords(const t_inputrec& inputRecord,
1535 bool havePartiallyFrozenAtoms,
1536 gmx::ArrayRef<const ParticleType> ptype,
1537 gmx::ArrayRef<const unsigned short> cFREEZE,
1538 gmx::ArrayRef<const unsigned short> cTC,
1539 gmx::ArrayRef<const real> invMass,
1540 gmx::ArrayRef<rvec> invMassPerDim,
1542 const gmx::ArrayRefWithPadding<const gmx::RVec>& f,
1543 const t_fcdata& fcdata,
1544 const gmx_ekindata_t* ekind,
1547 const t_commrec* cr,
1548 const bool haveConstraints)
1550 /* Running the velocity half does nothing except for velocity verlet */
1551 if ((updatePart == etrtVELOCITY1 || updatePart == etrtVELOCITY2) && !EI_VV(inputRecord.eI))
1553 gmx_incons("update_coords called for velocity without VV integrator");
1556 /* Cast to real for faster code, no loss in precision (see comment above) */
1557 real dt = inputRecord.delta_t;
1559 /* We need to update the NMR restraint history when time averaging is used */
1560 if (state->flags & enumValueToBitMask(StateEntry::DisreRm3Tav))
1562 update_disres_history(*fcdata.disres, &state->hist);
1564 if (state->flags & enumValueToBitMask(StateEntry::OrireDtav))
1566 update_orires_history(*fcdata.orires, &state->hist);
1569 /* ############# START The update of velocities and positions ######### */
1570 int nth = gmx_omp_nthreads_get(emntUpdate);
1572 #pragma omp parallel for num_threads(nth) schedule(static)
1573 for (int th = 0; th < nth; th++)
1577 int start_th, end_th;
1578 getThreadAtomRange(nth, th, homenr, &start_th, &end_th);
1580 const rvec* x_rvec = state->x.rvec_array();
1581 rvec* xp_rvec = xp_.rvec_array();
1582 rvec* v_rvec = state->v.rvec_array();
1583 const rvec* f_rvec = as_rvec_array(f.unpaddedConstArrayRef().data());
1585 switch (inputRecord.eI)
1587 case (IntegrationAlgorithm::MD):
1588 do_update_md(start_th,
1598 inputRecord.nsttcouple,
1599 inputRecord.nstpcouple,
1605 state->nosehoover_vxi.data(),
1607 havePartiallyFrozenAtoms);
1609 case (IntegrationAlgorithm::SD1):
1610 do_update_sd(start_th,
1618 gmx::arrayRefFromArray(inputRecord.opts.nFreeze, inputRecord.opts.ngfrz),
1623 inputRecord.ld_seed,
1628 case (IntegrationAlgorithm::BD):
1629 do_update_bd(start_th,
1637 gmx::arrayRefFromArray(inputRecord.opts.nFreeze, inputRecord.opts.ngfrz),
1642 inputRecord.bd_fric,
1644 inputRecord.ld_seed,
1645 DOMAINDECOMP(cr) ? cr->dd->globalAtomIndices.data() : nullptr);
1647 case (IntegrationAlgorithm::VV):
1648 case (IntegrationAlgorithm::VVAK):
1650 gmx_bool bExtended = (inputRecord.etc == TemperatureCoupling::NoseHoover
1651 || inputRecord.epc == PressureCoupling::ParrinelloRahman
1652 || inputRecord.epc == PressureCoupling::Mttk);
1654 /* assuming barostat coupled to group 0 */
1655 real alpha = 1.0 + DIM / static_cast<real>(inputRecord.opts.nrdf[0]);
1660 do_update_vv_vel(start_th,
1663 gmx::arrayRefFromArray(inputRecord.opts.nFreeze,
1664 inputRecord.opts.ngfrz),
1675 do_update_vv_pos(start_th,
1678 gmx::arrayRefFromArray(inputRecord.opts.nFreeze,
1679 inputRecord.opts.ngfrz),
1691 default: gmx_fatal(FARGS, "Don't know how to update coordinates");
1694 GMX_CATCH_ALL_AND_EXIT_WITH_FATAL_ERROR
1698 void Update::Impl::update_for_constraint_virial(const t_inputrec& inputRecord,
1700 bool havePartiallyFrozenAtoms,
1701 gmx::ArrayRef<real> invmass,
1702 gmx::ArrayRef<rvec> invMassPerDim,
1703 const t_state& state,
1704 const gmx::ArrayRefWithPadding<const gmx::RVec>& f,
1705 const gmx_ekindata_t& ekind)
1707 GMX_ASSERT(inputRecord.eI == IntegrationAlgorithm::MD || inputRecord.eI == IntegrationAlgorithm::SD1,
1708 "Only leap-frog is supported here");
1710 // Cast to real for faster code, no loss in precision
1711 const real dt = inputRecord.delta_t;
1713 const int nth = gmx_omp_nthreads_get(emntUpdate);
1715 #pragma omp parallel for num_threads(nth) schedule(static)
1716 for (int th = 0; th < nth; th++)
1720 int start_th, end_th;
1721 getThreadAtomRange(nth, th, homenr, &start_th, &end_th);
1723 const rvec* x_rvec = state.x.rvec_array();
1724 rvec* xp_rvec = xp_.rvec_array();
1725 const rvec* v_rvec = state.v.rvec_array();
1726 const rvec* f_rvec = as_rvec_array(f.unpaddedConstArrayRef().data());
1728 doUpdateMDDoNotUpdateVelocities(
1729 start_th, end_th, dt, x_rvec, xp_rvec, v_rvec, f_rvec, havePartiallyFrozenAtoms, invmass, invMassPerDim, ekind);
1731 GMX_CATCH_ALL_AND_EXIT_WITH_FATAL_ERROR