diff --git a/.gitignore b/.gitignore
index c75a8f8fa2c16b8c092ab1a361b003d1e3384032..812aa06dd54ee8bb81e87796deb8ee05160fec72 100644
--- a/.gitignore
+++ b/.gitignore
@@ -55,7 +55,9 @@ tests/brute_force_125_standard.dat
tests/swift_dopair_125_standard.dat
tests/brute_force_125_perturbed.dat
tests/swift_dopair_125_perturbed.dat
-tests/brute_force_active.dat
+tests/brute_force_pair_active.dat
+tests/brute_force_dopair2_active.dat
+tests/swift_dopair2_force_active.dat
tests/brute_force_periodic_BC_perturbed.dat
tests/swift_dopair_active.dat
tests/test_nonsym_density_serial.dat
diff --git a/README b/README
index c088a94488133ddf53cd8a6eba45d8dcdebfeb72..1ac1624b6a55fad43c73a8936b1a711ff956ca4d 100644
--- a/README
+++ b/README
@@ -20,7 +20,7 @@ Valid options are:
-C Run with cooling.
-d Dry run. Read the parameter file, allocate memory but does not read
the particles from ICs and exit before the start of time integration.
- Allows user to check validy of parameter and IC files as well as memory limits.
+ Allows user to check validity of parameter and IC files as well as memory limits.
-D Always drift all particles even the ones far from active particles. This emulates
Gadget-[23] and GIZMO's default behaviours.
-e Enable floating-point exceptions (debugging mode).
diff --git a/src/cache.h b/src/cache.h
index 22b79b1e49230c434a852da16512493e242ba3f9..3eb1e194dd4232319ac1d4a4323ca8099f044063 100644
--- a/src/cache.h
+++ b/src/cache.h
@@ -198,10 +198,7 @@ __attribute__((always_inline)) INLINE void cache_read_particles(
swift_declare_aligned_ptr(float, vz, ci_cache->vz, SWIFT_CACHE_ALIGNMENT);
const struct part *restrict parts = ci->parts;
- double loc[3];
- loc[0] = ci->loc[0];
- loc[1] = ci->loc[1];
- loc[2] = ci->loc[2];
+ const double loc[3] = {ci->loc[0], ci->loc[1], ci->loc[2]};
/* Shift the particles positions to a local frame so single precision can be
* used instead of double precision. */
@@ -210,7 +207,6 @@ __attribute__((always_inline)) INLINE void cache_read_particles(
y[i] = (float)(parts[i].x[1] - loc[1]);
z[i] = (float)(parts[i].x[2] - loc[2]);
h[i] = parts[i].h;
-
m[i] = parts[i].mass;
vx[i] = parts[i].v[0];
vy[i] = parts[i].v[1];
@@ -254,10 +250,7 @@ __attribute__((always_inline)) INLINE void cache_read_force_particles(
SWIFT_CACHE_ALIGNMENT);
const struct part *restrict parts = ci->parts;
- double loc[3];
- loc[0] = ci->loc[0];
- loc[1] = ci->loc[1];
- loc[2] = ci->loc[2];
+ const double loc[3] = {ci->loc[0], ci->loc[1], ci->loc[2]};
/* Shift the particles positions to a local frame so single precision can be
* used instead of double precision. */
@@ -266,12 +259,10 @@ __attribute__((always_inline)) INLINE void cache_read_force_particles(
y[i] = (float)(parts[i].x[1] - loc[1]);
z[i] = (float)(parts[i].x[2] - loc[2]);
h[i] = parts[i].h;
-
m[i] = parts[i].mass;
vx[i] = parts[i].v[0];
vy[i] = parts[i].v[1];
vz[i] = parts[i].v[2];
-
rho[i] = parts[i].rho;
grad_h[i] = parts[i].force.f;
pOrho2[i] = parts[i].force.P_over_rho2;
@@ -296,7 +287,6 @@ __attribute__((always_inline)) INLINE void cache_read_force_particles(
* @param shift The amount to shift the particle positions to account for BCs
* @param first_pi The first particle in cell ci that is in range.
* @param last_pj The last particle in cell cj that is in range.
- * @param num_vec_proc Number of vectors that will be used to process the
* interaction.
*/
__attribute__((always_inline)) INLINE void cache_read_two_partial_cells_sorted(
@@ -304,38 +294,39 @@ __attribute__((always_inline)) INLINE void cache_read_two_partial_cells_sorted(
struct cache *restrict const ci_cache,
struct cache *restrict const cj_cache, const struct entry *restrict sort_i,
const struct entry *restrict sort_j, const double *restrict const shift,
- int *first_pi, int *last_pj, const int num_vec_proc) {
+ int *first_pi, int *last_pj) {
+
+ /* Make the number of particles to be read a multiple of the vector size.
+ * This eliminates serial remainder loops where possible when populating the
+ * cache. */
- int idx;
- /* Pad number of particles read to the vector size. */
- int rem = (ci->count - *first_pi) % (num_vec_proc * VEC_SIZE);
+ /* Is the number of particles to read a multiple of the vector size? */
+ int rem = (ci->count - *first_pi) % VEC_SIZE;
if (rem != 0) {
- int pad = (num_vec_proc * VEC_SIZE) - rem;
+ int pad = VEC_SIZE - rem;
+ /* Decrease first_pi if there are particles in the cell left to read. */
if (*first_pi - pad >= 0) *first_pi -= pad;
}
- rem = *last_pj % (num_vec_proc * VEC_SIZE);
+ rem = (*last_pj + 1) % VEC_SIZE;
if (rem != 0) {
- int pad = (num_vec_proc * VEC_SIZE) - rem;
+ int pad = VEC_SIZE - rem;
+ /* Increase last_pj if there are particles in the cell left to read. */
if (*last_pj + pad < cj->count) *last_pj += pad;
}
- int first_pi_align = *first_pi;
- int last_pj_align = *last_pj;
+ /* Get some local pointers */
+ const int first_pi_align = *first_pi;
+ const int last_pj_align = *last_pj;
const struct part *restrict parts_i = ci->parts;
const struct part *restrict parts_j = cj->parts;
- double loc[3];
- loc[0] = cj->loc[0];
- loc[1] = cj->loc[1];
- loc[2] = cj->loc[2];
- /* Shift ci particles for boundary conditions and location of cell.*/
- double total_ci_shift[3];
- total_ci_shift[0] = loc[0] + shift[0];
- total_ci_shift[1] = loc[1] + shift[1];
- total_ci_shift[2] = loc[2] + shift[2];
+ /* Shift particles to the local frame and account for boundary conditions.*/
+ const double total_ci_shift[3] = {
+ cj->loc[0] + shift[0], cj->loc[1] + shift[1], cj->loc[2] + shift[2]};
+ const double total_cj_shift[3] = {cj->loc[0], cj->loc[1], cj->loc[2]};
/* Let the compiler know that the data is aligned and create pointers to the
* arrays inside the cache. */
@@ -349,19 +340,15 @@ __attribute__((always_inline)) INLINE void cache_read_two_partial_cells_sorted(
swift_declare_aligned_ptr(float, vz, ci_cache->vz, SWIFT_CACHE_ALIGNMENT);
int ci_cache_count = ci->count - first_pi_align;
+
/* Shift the particles positions to a local frame (ci frame) so single
- * precision
- * can be
- * used instead of double precision. Also shift the cell ci, particles
- * positions
- * due to BCs but leave cell cj. */
+ * precision can be used instead of double precision. */
for (int i = 0; i < ci_cache_count; i++) {
- idx = sort_i[i + first_pi_align].i;
+ const int idx = sort_i[i + first_pi_align].i;
x[i] = (float)(parts_i[idx].x[0] - total_ci_shift[0]);
y[i] = (float)(parts_i[idx].x[1] - total_ci_shift[1]);
z[i] = (float)(parts_i[idx].x[2] - total_ci_shift[2]);
h[i] = parts_i[idx].h;
-
m[i] = parts_i[idx].mass;
vx[i] = parts_i[idx].v[0];
vy[i] = parts_i[idx].v[1];
@@ -384,36 +371,42 @@ __attribute__((always_inline)) INLINE void cache_read_two_partial_cells_sorted(
"is not within "
"[-4*ci->width*(1 + 2*space_maxreldx), 4*ci->width*(1 + "
"2*space_maxreldx)]. x=%f, ci->width[0]=%f",
- ci->loc[0], ci->loc[1], ci->loc[2], loc[0], loc[1], loc[2], i, x[i],
- ci->width[0]);
+ ci->loc[0], ci->loc[1], ci->loc[2], cj->loc[0], cj->loc[1],
+ cj->loc[2], i, x[i], ci->width[0]);
if (y[i] > shift_threshold_y || y[i] < -shift_threshold_y)
error(
"Error: ci->loc[%lf,%lf,%lf], cj->loc[%lf,%lf,%lf] Particle %d y pos "
"is not within "
"[-4*ci->width*(1 + 2*space_maxreldx), 4*ci->width*(1 + "
"2*space_maxreldx)]. y=%f, ci->width[1]=%f",
- ci->loc[0], ci->loc[1], ci->loc[2], loc[0], loc[1], loc[2], i, y[i],
- ci->width[1]);
+ ci->loc[0], ci->loc[1], ci->loc[2], cj->loc[0], cj->loc[1],
+ cj->loc[2], i, y[i], ci->width[1]);
if (z[i] > shift_threshold_z || z[i] < -shift_threshold_z)
error(
"Error: ci->loc[%lf,%lf,%lf], cj->loc[%lf,%lf,%lf] Particle %d z pos "
"is not within "
"[-4*ci->width*(1 + 2*space_maxreldx), 4*ci->width*(1 + "
"2*space_maxreldx)]. z=%f, ci->width[2]=%f",
- ci->loc[0], ci->loc[1], ci->loc[2], loc[0], loc[1], loc[2], i, z[i],
- ci->width[2]);
+ ci->loc[0], ci->loc[1], ci->loc[2], cj->loc[0], cj->loc[1],
+ cj->loc[2], i, z[i], ci->width[2]);
}
#endif
/* Pad cache with fake particles that exist outside the cell so will not
- * interact.*/
- float fake_pix = 2.0f * parts_i[sort_i[ci->count - 1].i].x[0];
+ * interact. We use values of the same magnitude (but negative!) as the real
+ * particles to avoid overflow problems. */
+ const double max_dx = max(ci->dx_max_part, cj->dx_max_part);
+ const float pos_padded[3] = {-(2. * ci->width[0] + max_dx),
+ -(2. * ci->width[1] + max_dx),
+ -(2. * ci->width[2] + max_dx)};
+ const float h_padded = ci->parts[0].h;
+
for (int i = ci->count - first_pi_align;
i < ci->count - first_pi_align + VEC_SIZE; i++) {
- x[i] = fake_pix;
- y[i] = 1.f;
- z[i] = 1.f;
- h[i] = 1.f;
+ x[i] = pos_padded[0];
+ y[i] = pos_padded[1];
+ z[i] = pos_padded[2];
+ h[i] = h_padded;
m[i] = 1.f;
vx[i] = 1.f;
@@ -433,12 +426,11 @@ __attribute__((always_inline)) INLINE void cache_read_two_partial_cells_sorted(
swift_declare_aligned_ptr(float, vzj, cj_cache->vz, SWIFT_CACHE_ALIGNMENT);
for (int i = 0; i <= last_pj_align; i++) {
- idx = sort_j[i].i;
- xj[i] = (float)(parts_j[idx].x[0] - loc[0]);
- yj[i] = (float)(parts_j[idx].x[1] - loc[1]);
- zj[i] = (float)(parts_j[idx].x[2] - loc[2]);
+ const int idx = sort_j[i].i;
+ xj[i] = (float)(parts_j[idx].x[0] - total_cj_shift[0]);
+ yj[i] = (float)(parts_j[idx].x[1] - total_cj_shift[1]);
+ zj[i] = (float)(parts_j[idx].x[2] - total_cj_shift[2]);
hj[i] = parts_j[idx].h;
-
mj[i] = parts_j[idx].mass;
vxj[i] = parts_j[idx].v[0];
vyj[i] = parts_j[idx].v[1];
@@ -454,40 +446,228 @@ __attribute__((always_inline)) INLINE void cache_read_two_partial_cells_sorted(
"pos is not within "
"[-4*ci->width*(1 + 2*space_maxreldx), 4*ci->width*(1 + "
"2*space_maxreldx)]. xj=%f, ci->width[0]=%f",
- ci->loc[0], ci->loc[1], ci->loc[2], loc[0], loc[1], loc[2], i, xj[i],
- ci->width[0]);
+ ci->loc[0], ci->loc[1], ci->loc[2], cj->loc[0], cj->loc[1],
+ cj->loc[2], i, xj[i], ci->width[0]);
if (yj[i] > shift_threshold_y || yj[i] < -shift_threshold_y)
error(
"Error: ci->loc[%lf,%lf,%lf], cj->loc[%lf,%lf,%lf] Particle %d yj "
"pos is not within "
"[-4*ci->width*(1 + 2*space_maxreldx), 4*ci->width*(1 + "
"2*space_maxreldx)]. yj=%f, ci->width[1]=%f",
- ci->loc[0], ci->loc[1], ci->loc[2], loc[0], loc[1], loc[2], i, yj[i],
- ci->width[1]);
+ ci->loc[0], ci->loc[1], ci->loc[2], cj->loc[0], cj->loc[1],
+ cj->loc[2], i, yj[i], ci->width[1]);
if (zj[i] > shift_threshold_z || zj[i] < -shift_threshold_z)
error(
"Error: ci->loc[%lf,%lf,%lf], cj->loc[%lf,%lf,%lf] Particle %d zj "
"pos is not within "
"[-4*ci->width*(1 + 2*space_maxreldx), 4*ci->width*(1 + "
"2*space_maxreldx)]. zj=%f, ci->width[2]=%f",
- ci->loc[0], ci->loc[1], ci->loc[2], loc[0], loc[1], loc[2], i, zj[i],
- ci->width[2]);
+ ci->loc[0], ci->loc[1], ci->loc[2], cj->loc[0], cj->loc[1],
+ cj->loc[2], i, zj[i], ci->width[2]);
}
#endif
/* Pad cache with fake particles that exist outside the cell so will not
- * interact.*/
- float fake_pjx = 2.0f * cj->parts[sort_j[cj->count - 1].i].x[0];
+ * interact. We use values of the same magnitude (but negative!) as the real
+ * particles to avoid overflow problems. */
+ const float pos_padded_j[3] = {-(2. * cj->width[0] + max_dx),
+ -(2. * cj->width[1] + max_dx),
+ -(2. * cj->width[2] + max_dx)};
+ const float h_padded_j = cj->parts[0].h;
+
for (int i = last_pj_align + 1; i < last_pj_align + 1 + VEC_SIZE; i++) {
- xj[i] = fake_pjx;
- yj[i] = 1.f;
- zj[i] = 1.f;
- hj[i] = 1.f;
+ xj[i] = pos_padded_j[0];
+ yj[i] = pos_padded_j[1];
+ zj[i] = pos_padded_j[2];
+ hj[i] = h_padded_j;
+ mj[i] = 1.f;
+ vxj[i] = 1.f;
+ vyj[i] = 1.f;
+ vzj[i] = 1.f;
+ }
+}
+
+/**
+ * @brief Populate caches by only reading particles that are within range of
+ * each other within the adjoining cell.Also read the particles into the cache
+ * in sorted order.
+ *
+ * @param ci The i #cell.
+ * @param cj The j #cell.
+ * @param ci_cache The #cache for cell ci.
+ * @param cj_cache The #cache for cell cj.
+ * @param sort_i The array of sorted particle indices for cell ci.
+ * @param sort_j The array of sorted particle indices for cell ci.
+ * @param shift The amount to shift the particle positions to account for BCs
+ * @param first_pi The first particle in cell ci that is in range.
+ * @param last_pj The last particle in cell cj that is in range.
+ * interaction.
+ */
+__attribute__((always_inline)) INLINE void
+cache_read_two_partial_cells_sorted_force(
+ const struct cell *const ci, const struct cell *const cj,
+ struct cache *const ci_cache, struct cache *const cj_cache,
+ const struct entry *restrict sort_i, const struct entry *restrict sort_j,
+ const double *const shift, int *first_pi, int *last_pj) {
+
+ /* Make the number of particles to be read a multiple of the vector size.
+ * This eliminates serial remainder loops where possible when populating the
+ * cache. */
+
+ /* Is the number of particles to read a multiple of the vector size? */
+ int rem = (ci->count - *first_pi) % VEC_SIZE;
+ if (rem != 0) {
+ int pad = VEC_SIZE - rem;
+
+ /* Decrease first_pi if there are particles in the cell left to read. */
+ if (*first_pi - pad >= 0) *first_pi -= pad;
+ }
+
+ rem = (*last_pj + 1) % VEC_SIZE;
+ if (rem != 0) {
+ int pad = VEC_SIZE - rem;
+
+ /* Increase last_pj if there are particles in the cell left to read. */
+ if (*last_pj + pad < cj->count) *last_pj += pad;
+ }
+
+ /* Get some local pointers */
+ const int first_pi_align = *first_pi;
+ const int last_pj_align = *last_pj;
+ const struct part *restrict parts_i = ci->parts;
+ const struct part *restrict parts_j = cj->parts;
+
+ /* Shift particles to the local frame and account for boundary conditions.*/
+ const double total_ci_shift[3] = {
+ cj->loc[0] + shift[0], cj->loc[1] + shift[1], cj->loc[2] + shift[2]};
+ const double total_cj_shift[3] = {cj->loc[0], cj->loc[1], cj->loc[2]};
+
+ /* Let the compiler know that the data is aligned and create pointers to the
+ * arrays inside the cache. */
+ swift_declare_aligned_ptr(float, x, ci_cache->x, SWIFT_CACHE_ALIGNMENT);
+ swift_declare_aligned_ptr(float, y, ci_cache->y, SWIFT_CACHE_ALIGNMENT);
+ swift_declare_aligned_ptr(float, z, ci_cache->z, SWIFT_CACHE_ALIGNMENT);
+ swift_declare_aligned_ptr(float, h, ci_cache->h, SWIFT_CACHE_ALIGNMENT);
+ swift_declare_aligned_ptr(float, m, ci_cache->m, SWIFT_CACHE_ALIGNMENT);
+ swift_declare_aligned_ptr(float, vx, ci_cache->vx, SWIFT_CACHE_ALIGNMENT);
+ swift_declare_aligned_ptr(float, vy, ci_cache->vy, SWIFT_CACHE_ALIGNMENT);
+ swift_declare_aligned_ptr(float, vz, ci_cache->vz, SWIFT_CACHE_ALIGNMENT);
+ swift_declare_aligned_ptr(float, rho, ci_cache->rho, SWIFT_CACHE_ALIGNMENT);
+ swift_declare_aligned_ptr(float, grad_h, ci_cache->grad_h,
+ SWIFT_CACHE_ALIGNMENT);
+ swift_declare_aligned_ptr(float, pOrho2, ci_cache->pOrho2,
+ SWIFT_CACHE_ALIGNMENT);
+ swift_declare_aligned_ptr(float, balsara, ci_cache->balsara,
+ SWIFT_CACHE_ALIGNMENT);
+ swift_declare_aligned_ptr(float, soundspeed, ci_cache->soundspeed,
+ SWIFT_CACHE_ALIGNMENT);
+
+ int ci_cache_count = ci->count - first_pi_align;
+ /* Shift the particles positions to a local frame (ci frame) so single
+ * precision can be used instead of double precision. */
+ for (int i = 0; i < ci_cache_count; i++) {
+
+ const int idx = sort_i[i + first_pi_align].i;
+ x[i] = (float)(parts_i[idx].x[0] - total_ci_shift[0]);
+ y[i] = (float)(parts_i[idx].x[1] - total_ci_shift[1]);
+ z[i] = (float)(parts_i[idx].x[2] - total_ci_shift[2]);
+ h[i] = parts_i[idx].h;
+ m[i] = parts_i[idx].mass;
+ vx[i] = parts_i[idx].v[0];
+ vy[i] = parts_i[idx].v[1];
+ vz[i] = parts_i[idx].v[2];
+ rho[i] = parts_i[idx].rho;
+ grad_h[i] = parts_i[idx].force.f;
+ pOrho2[i] = parts_i[idx].force.P_over_rho2;
+ balsara[i] = parts_i[idx].force.balsara;
+ soundspeed[i] = parts_i[idx].force.soundspeed;
+ }
+
+ /* Pad cache with fake particles that exist outside the cell so will not
+ * interact. We use values of the same magnitude (but negative!) as the real
+ * particles to avoid overflow problems. */
+ const double max_dx = max(ci->dx_max_part, cj->dx_max_part);
+ const float pos_padded[3] = {-(2. * ci->width[0] + max_dx),
+ -(2. * ci->width[1] + max_dx),
+ -(2. * ci->width[2] + max_dx)};
+ const float h_padded = ci->parts[0].h;
+
+ for (int i = ci->count - first_pi_align;
+ i < ci->count - first_pi_align + VEC_SIZE; i++) {
+ x[i] = pos_padded[0];
+ y[i] = pos_padded[1];
+ z[i] = pos_padded[2];
+ h[i] = h_padded;
+ m[i] = 1.f;
+ vx[i] = 1.f;
+ vy[i] = 1.f;
+ vz[i] = 1.f;
+ rho[i] = 1.f;
+ grad_h[i] = 1.f;
+ pOrho2[i] = 1.f;
+ balsara[i] = 1.f;
+ soundspeed[i] = 1.f;
+ }
+
+ /* Let the compiler know that the data is aligned and create pointers to the
+ * arrays inside the cache. */
+ swift_declare_aligned_ptr(float, xj, cj_cache->x, SWIFT_CACHE_ALIGNMENT);
+ swift_declare_aligned_ptr(float, yj, cj_cache->y, SWIFT_CACHE_ALIGNMENT);
+ swift_declare_aligned_ptr(float, zj, cj_cache->z, SWIFT_CACHE_ALIGNMENT);
+ swift_declare_aligned_ptr(float, hj, cj_cache->h, SWIFT_CACHE_ALIGNMENT);
+ swift_declare_aligned_ptr(float, mj, cj_cache->m, SWIFT_CACHE_ALIGNMENT);
+ swift_declare_aligned_ptr(float, vxj, cj_cache->vx, SWIFT_CACHE_ALIGNMENT);
+ swift_declare_aligned_ptr(float, vyj, cj_cache->vy, SWIFT_CACHE_ALIGNMENT);
+ swift_declare_aligned_ptr(float, vzj, cj_cache->vz, SWIFT_CACHE_ALIGNMENT);
+ swift_declare_aligned_ptr(float, rhoj, cj_cache->rho, SWIFT_CACHE_ALIGNMENT);
+ swift_declare_aligned_ptr(float, grad_hj, cj_cache->grad_h,
+ SWIFT_CACHE_ALIGNMENT);
+ swift_declare_aligned_ptr(float, pOrho2j, cj_cache->pOrho2,
+ SWIFT_CACHE_ALIGNMENT);
+ swift_declare_aligned_ptr(float, balsaraj, cj_cache->balsara,
+ SWIFT_CACHE_ALIGNMENT);
+ swift_declare_aligned_ptr(float, soundspeedj, cj_cache->soundspeed,
+ SWIFT_CACHE_ALIGNMENT);
+
+ for (int i = 0; i <= last_pj_align; i++) {
+ const int idx = sort_j[i].i;
+ xj[i] = (float)(parts_j[idx].x[0] - total_cj_shift[0]);
+ yj[i] = (float)(parts_j[idx].x[1] - total_cj_shift[1]);
+ zj[i] = (float)(parts_j[idx].x[2] - total_cj_shift[2]);
+ hj[i] = parts_j[idx].h;
+ mj[i] = parts_j[idx].mass;
+ vxj[i] = parts_j[idx].v[0];
+ vyj[i] = parts_j[idx].v[1];
+ vzj[i] = parts_j[idx].v[2];
+ rhoj[i] = parts_j[idx].rho;
+ grad_hj[i] = parts_j[idx].force.f;
+ pOrho2j[i] = parts_j[idx].force.P_over_rho2;
+ balsaraj[i] = parts_j[idx].force.balsara;
+ soundspeedj[i] = parts_j[idx].force.soundspeed;
+ }
+ /* Pad cache with fake particles that exist outside the cell so will not
+ * interact. We use values of the same magnitude (but negative!) as the real
+ * particles to avoid overflow problems. */
+ const float pos_padded_j[3] = {-(2. * cj->width[0] + max_dx),
+ -(2. * cj->width[1] + max_dx),
+ -(2. * cj->width[2] + max_dx)};
+ const float h_padded_j = cj->parts[0].h;
+
+ for (int i = last_pj_align + 1; i < last_pj_align + 1 + VEC_SIZE; i++) {
+ xj[i] = pos_padded_j[0];
+ yj[i] = pos_padded_j[1];
+ zj[i] = pos_padded_j[2];
+ hj[i] = h_padded_j;
mj[i] = 1.f;
vxj[i] = 1.f;
vyj[i] = 1.f;
vzj[i] = 1.f;
+ rhoj[i] = 1.f;
+ grad_hj[i] = 1.f;
+ pOrho2j[i] = 1.f;
+ balsaraj[i] = 1.f;
+ soundspeedj[i] = 1.f;
}
}
@@ -506,6 +686,11 @@ static INLINE void cache_clean(struct cache *c) {
free(c->vz);
free(c->h);
free(c->max_index);
+ free(c->rho);
+ free(c->grad_h);
+ free(c->pOrho2);
+ free(c->balsara);
+ free(c->soundspeed);
}
}
diff --git a/src/hydro/Gadget2/hydro_iact.h b/src/hydro/Gadget2/hydro_iact.h
index 3851dd6e894eafff29d35942ab0f364b5919e029..666e0be835f114959f2f2a074900700b383e10fe 100644
--- a/src/hydro/Gadget2/hydro_iact.h
+++ b/src/hydro/Gadget2/hydro_iact.h
@@ -170,17 +170,15 @@ runner_iact_nonsym_1_vec_density(vector *r2, vector *dx, vector *dy, vector *dz,
mask_t mask) {
vector r, ri, ui, wi, wi_dx;
- vector mj;
vector dvx, dvy, dvz;
- vector vjx, vjy, vjz;
vector dvdr;
vector curlvrx, curlvry, curlvrz;
/* Fill the vectors. */
- mj.v = vec_load(Mj);
- vjx.v = vec_load(Vjx);
- vjy.v = vec_load(Vjy);
- vjz.v = vec_load(Vjz);
+ const vector mj = vector_load(Mj);
+ const vector vjx = vector_load(Vjx);
+ const vector vjy = vector_load(Vjy);
+ const vector vjz = vector_load(Vjz);
/* Get the radius and inverse radius. */
ri = vec_reciprocal_sqrt(*r2);
@@ -245,38 +243,34 @@ runner_iact_nonsym_2_vec_density(float *R2, float *Dx, float *Dy, float *Dz,
vector *curlvySum, vector *curlvzSum,
mask_t mask, mask_t mask2, short mask_cond) {
- vector r, ri, r2, ui, wi, wi_dx;
- vector mj;
- vector dx, dy, dz, dvx, dvy, dvz;
- vector vjx, vjy, vjz;
+ vector r, ri, ui, wi, wi_dx;
+ vector dvx, dvy, dvz;
vector dvdr;
vector curlvrx, curlvry, curlvrz;
- vector r_2, ri2, r2_2, ui2, wi2, wi_dx2;
- vector mj2;
- vector dx2, dy2, dz2, dvx2, dvy2, dvz2;
- vector vjx2, vjy2, vjz2;
+ vector r_2, ri2, ui2, wi2, wi_dx2;
+ vector dvx2, dvy2, dvz2;
vector dvdr2;
vector curlvrx2, curlvry2, curlvrz2;
/* Fill the vectors. */
- mj.v = vec_load(Mj);
- mj2.v = vec_load(&Mj[VEC_SIZE]);
- vjx.v = vec_load(Vjx);
- vjx2.v = vec_load(&Vjx[VEC_SIZE]);
- vjy.v = vec_load(Vjy);
- vjy2.v = vec_load(&Vjy[VEC_SIZE]);
- vjz.v = vec_load(Vjz);
- vjz2.v = vec_load(&Vjz[VEC_SIZE]);
- dx.v = vec_load(Dx);
- dx2.v = vec_load(&Dx[VEC_SIZE]);
- dy.v = vec_load(Dy);
- dy2.v = vec_load(&Dy[VEC_SIZE]);
- dz.v = vec_load(Dz);
- dz2.v = vec_load(&Dz[VEC_SIZE]);
+ const vector mj = vector_load(Mj);
+ const vector mj2 = vector_load(&Mj[VEC_SIZE]);
+ const vector vjx = vector_load(Vjx);
+ const vector vjx2 = vector_load(&Vjx[VEC_SIZE]);
+ const vector vjy = vector_load(Vjy);
+ const vector vjy2 = vector_load(&Vjy[VEC_SIZE]);
+ const vector vjz = vector_load(Vjz);
+ const vector vjz2 = vector_load(&Vjz[VEC_SIZE]);
+ const vector dx = vector_load(Dx);
+ const vector dx2 = vector_load(&Dx[VEC_SIZE]);
+ const vector dy = vector_load(Dy);
+ const vector dy2 = vector_load(&Dy[VEC_SIZE]);
+ const vector dz = vector_load(Dz);
+ const vector dz2 = vector_load(&Dz[VEC_SIZE]);
/* Get the radius and inverse radius. */
- r2.v = vec_load(R2);
- r2_2.v = vec_load(&R2[VEC_SIZE]);
+ const vector r2 = vector_load(R2);
+ const vector r2_2 = vector_load(&R2[VEC_SIZE]);
ri = vec_reciprocal_sqrt(r2);
ri2 = vec_reciprocal_sqrt(r2_2);
r.v = vec_mul(r2.v, ri.v);
@@ -592,30 +586,29 @@ runner_iact_nonsym_1_vec_force(
#ifdef WITH_VECTORIZATION
vector r, ri;
- vector vjx, vjy, vjz, dvx, dvy, dvz;
- vector pjrho, grad_hj, pjPOrho2, balsara_j, cj, mj;
+ vector dvx, dvy, dvz;
vector xi, xj;
vector hid_inv, hjd_inv;
vector wi_dx, wj_dx, wi_dr, wj_dr, dvdr;
vector piax, piay, piaz;
vector pih_dt;
vector v_sig;
- vector omega_ij, mu_ij, fac_mu, balsara;
+ vector omega_ij, mu_ij, balsara;
vector rho_ij, visc, visc_term, sph_term, acc, entropy_dt;
/* Fill vectors. */
- vjx.v = vec_load(Vjx);
- vjy.v = vec_load(Vjy);
- vjz.v = vec_load(Vjz);
- mj.v = vec_load(Mj);
-
- pjrho.v = vec_load(Pjrho);
- grad_hj.v = vec_load(Grad_hj);
- pjPOrho2.v = vec_load(PjPOrho2);
- balsara_j.v = vec_load(Balsara_j);
- cj.v = vec_load(Cj);
-
- fac_mu.v = vec_set1(1.f); /* Will change with cosmological integration */
+ const vector vjx = vector_load(Vjx);
+ const vector vjy = vector_load(Vjy);
+ const vector vjz = vector_load(Vjz);
+ const vector mj = vector_load(Mj);
+ const vector pjrho = vector_load(Pjrho);
+ const vector grad_hj = vector_load(Grad_hj);
+ const vector pjPOrho2 = vector_load(PjPOrho2);
+ const vector balsara_j = vector_load(Balsara_j);
+ const vector cj = vector_load(Cj);
+
+ const vector fac_mu =
+ vector_set1(1.f); /* Will change with cosmological integration */
/* Load stuff. */
balsara.v = vec_add(balsara_i.v, balsara_j.v);
@@ -634,7 +627,7 @@ runner_iact_nonsym_1_vec_force(
hjd_inv = pow_dimension_plus_one_vec(hj_inv);
xj.v = vec_mul(r.v, hj_inv.v);
- /* Calculate the kernel for two particles. */
+ /* Calculate the kernel. */
kernel_eval_dWdx_force_vec(&xj, &wj_dx);
wj_dr.v = vec_mul(hjd_inv.v, wj_dx.v);
@@ -720,23 +713,19 @@ runner_iact_nonsym_2_vec_force(
#ifdef WITH_VECTORIZATION
- vector r, r2, ri;
- vector dx, dy, dz, dvx, dvy, dvz;
- vector vjx, vjy, vjz;
- vector pjrho, grad_hj, pjPOrho2, balsara_j, cj, mj, hj_inv;
+ vector r, ri;
+ vector dvx, dvy, dvz;
vector ui, uj;
vector hid_inv, hjd_inv;
vector wi_dx, wj_dx, wi_dr, wj_dr, dvdr;
vector piax, piay, piaz;
vector pih_dt;
vector v_sig;
- vector omega_ij, mu_ij, fac_mu, balsara;
+ vector omega_ij, mu_ij, balsara;
vector rho_ij, visc, visc_term, sph_term, acc, entropy_dt;
- vector r_2, r2_2, ri_2;
- vector dx_2, dy_2, dz_2, dvx_2, dvy_2, dvz_2;
- vector vjx_2, vjy_2, vjz_2;
- vector pjrho_2, grad_hj_2, pjPOrho2_2, balsara_j_2, cj_2, mj_2, hj_inv_2;
+ vector r_2, ri_2;
+ vector dvx_2, dvy_2, dvz_2;
vector ui_2, uj_2;
vector hjd_inv_2;
vector wi_dx_2, wj_dx_2, wi_dr_2, wj_dr_2, dvdr_2;
@@ -747,44 +736,45 @@ runner_iact_nonsym_2_vec_force(
vector rho_ij_2, visc_2, visc_term_2, sph_term_2, acc_2, entropy_dt_2;
/* Fill vectors. */
- mj.v = vec_load(Mj);
- mj_2.v = vec_load(&Mj[VEC_SIZE]);
- vjx.v = vec_load(Vjx);
- vjx_2.v = vec_load(&Vjx[VEC_SIZE]);
- vjy.v = vec_load(Vjy);
- vjy_2.v = vec_load(&Vjy[VEC_SIZE]);
- vjz.v = vec_load(Vjz);
- vjz_2.v = vec_load(&Vjz[VEC_SIZE]);
- dx.v = vec_load(Dx);
- dx_2.v = vec_load(&Dx[VEC_SIZE]);
- dy.v = vec_load(Dy);
- dy_2.v = vec_load(&Dy[VEC_SIZE]);
- dz.v = vec_load(Dz);
- dz_2.v = vec_load(&Dz[VEC_SIZE]);
+ const vector mj = vector_load(Mj);
+ const vector mj_2 = vector_load(&Mj[VEC_SIZE]);
+ const vector vjx = vector_load(Vjx);
+ const vector vjx_2 = vector_load(&Vjx[VEC_SIZE]);
+ const vector vjy = vector_load(Vjy);
+ const vector vjy_2 = vector_load(&Vjy[VEC_SIZE]);
+ const vector vjz = vector_load(Vjz);
+ const vector vjz_2 = vector_load(&Vjz[VEC_SIZE]);
+ const vector dx = vector_load(Dx);
+ const vector dx_2 = vector_load(&Dx[VEC_SIZE]);
+ const vector dy = vector_load(Dy);
+ const vector dy_2 = vector_load(&Dy[VEC_SIZE]);
+ const vector dz = vector_load(Dz);
+ const vector dz_2 = vector_load(&Dz[VEC_SIZE]);
/* Get the radius and inverse radius. */
- r2.v = vec_load(R2);
- r2_2.v = vec_load(&R2[VEC_SIZE]);
+ const vector r2 = vector_load(R2);
+ const vector r2_2 = vector_load(&R2[VEC_SIZE]);
ri = vec_reciprocal_sqrt(r2);
ri_2 = vec_reciprocal_sqrt(r2_2);
r.v = vec_mul(r2.v, ri.v);
r_2.v = vec_mul(r2_2.v, ri_2.v);
/* Get remaining properties. */
- pjrho.v = vec_load(Pjrho);
- pjrho_2.v = vec_load(&Pjrho[VEC_SIZE]);
- grad_hj.v = vec_load(Grad_hj);
- grad_hj_2.v = vec_load(&Grad_hj[VEC_SIZE]);
- pjPOrho2.v = vec_load(PjPOrho2);
- pjPOrho2_2.v = vec_load(&PjPOrho2[VEC_SIZE]);
- balsara_j.v = vec_load(Balsara_j);
- balsara_j_2.v = vec_load(&Balsara_j[VEC_SIZE]);
- cj.v = vec_load(Cj);
- cj_2.v = vec_load(&Cj[VEC_SIZE]);
- hj_inv.v = vec_load(Hj_inv);
- hj_inv_2.v = vec_load(&Hj_inv[VEC_SIZE]);
-
- fac_mu.v = vec_set1(1.f); /* Will change with cosmological integration */
+ const vector pjrho = vector_load(Pjrho);
+ const vector pjrho_2 = vector_load(&Pjrho[VEC_SIZE]);
+ const vector grad_hj = vector_load(Grad_hj);
+ const vector grad_hj_2 = vector_load(&Grad_hj[VEC_SIZE]);
+ const vector pjPOrho2 = vector_load(PjPOrho2);
+ const vector pjPOrho2_2 = vector_load(&PjPOrho2[VEC_SIZE]);
+ const vector balsara_j = vector_load(Balsara_j);
+ const vector balsara_j_2 = vector_load(&Balsara_j[VEC_SIZE]);
+ const vector cj = vector_load(Cj);
+ const vector cj_2 = vector_load(&Cj[VEC_SIZE]);
+ const vector hj_inv = vector_load(Hj_inv);
+ const vector hj_inv_2 = vector_load(&Hj_inv[VEC_SIZE]);
+
+ const vector fac_mu =
+ vector_set1(1.f); /* Will change with cosmological integration */
/* Find the balsara switch. */
balsara.v = vec_add(balsara_i.v, balsara_j.v);
diff --git a/src/parallel_io.c b/src/parallel_io.c
index 65f8fc9c20b1856a9c2f72625fb3bba0c8f7be8e..26686baadb7c040264c20385d0c89cb30e5dc398 100644
--- a/src/parallel_io.c
+++ b/src/parallel_io.c
@@ -51,24 +51,19 @@
#include "units.h"
#include "xmf.h"
+/* The current limit of ROMIO (the underlying MPI-IO layer) is 2GB */
+#define HDF5_PARALLEL_IO_MAX_BYTES 2000000000LL
+
/**
* @brief Reads a data array from a given HDF5 group.
*
* @param grp The group from which to read.
- * @param name The name of the array to read.
- * @param type The #DATA_TYPE of the attribute.
- * @param N The number of particles.
- * @param dim The dimension of the data (1 for scalar, 3 for vector)
- * @param part_c A (char*) pointer on the first occurrence of the field of
- *interest in the parts array
- * @param importance If COMPULSORY, the data must be present in the IC file. If
- *OPTIONAL, the array will be zeroed when the data is not present.
- *
- * @todo A better version using HDF5 hyper-slabs to read the file directly into
- *the part array
- * will be written once the structures have been stabilized.
- *
- * Calls #error() if an error occurs.
+ * @param prop The #io_props of the field to read.
+ * @param N The number of particles on that rank.
+ * @param N_total The total number of particles.
+ * @param offset The offset in the array on disk for this rank.
+ * @param internal_units The #unit_system used internally.
+ * @param ic_units The #unit_system used in the ICs.
*/
void readArray(hid_t grp, const struct io_props prop, size_t N,
long long N_total, long long offset,
@@ -183,36 +178,34 @@ void readArray(hid_t grp, const struct io_props prop, size_t N,
*-----------------------------------------------------------------------------*/
/**
- * @brief Writes a data array in given HDF5 group.
+ * @brief Writes a chunk of data in an open HDF5 dataset
*
* @param e The #engine we are writing from.
- * @param grp The group in which to write.
- * @param fileName The name of the file in which the data is written
- * @param xmfFile The FILE used to write the XMF description
+ * @param h_data The HDF5 dataset to write to.
+ * @param h_plist_id the parallel HDF5 properties.
+ * @param props The #io_props of the field to read.
* @param N The number of particles to write.
- * @param N_total Total number of particles across all cores
- * @param offset Offset in the array where this mpi task starts writing
- * @param internal_units The #unit_system used internally
- * @param snapshot_units The #unit_system used in the snapshots
- *
- * @todo A better version using HDF5 hyper-slabs to write the file directly from
- * the part array will be written once the structures have been stabilized.
- *
+ * @param offset Offset in the array where this mpi task starts writing.
+ * @param internal_units The #unit_system used internally.
+ * @param snapshot_units The #unit_system used in the snapshots.
*/
-void writeArray(struct engine* e, hid_t grp, char* fileName, FILE* xmfFile,
- char* partTypeGroupName, const struct io_props props, size_t N,
- long long N_total, int mpi_rank, long long offset,
- const struct unit_system* internal_units,
- const struct unit_system* snapshot_units) {
+void writeArray_chunk(struct engine* e, hid_t h_data, hid_t h_plist_id,
+ const struct io_props props, size_t N, long long offset,
+ const struct unit_system* internal_units,
+ const struct unit_system* snapshot_units) {
const size_t typeSize = io_sizeof_type(props.type);
const size_t copySize = typeSize * props.dimension;
const size_t num_elements = N * props.dimension;
+ /* Can't handle writes of more than 2GB */
+ if (N * props.dimension * typeSize > HDF5_PARALLEL_IO_MAX_BYTES)
+ error("Dataset too large to be written in one pass!");
+
/* message("Writing '%s' array...", props.name); */
/* Allocate temporary buffer */
- void* temp = malloc(num_elements * io_sizeof_type(props.type));
+ void* temp = malloc(num_elements * typeSize);
if (temp == NULL) error("Unable to allocate memory for temporary buffer");
/* Copy particle data to temporary buffer */
@@ -259,29 +252,19 @@ void writeArray(struct engine* e, hid_t grp, char* fileName, FILE* xmfFile,
props.name);
}
- hid_t h_filespace = H5Screate(H5S_SIMPLE);
- if (h_filespace < 0) {
- error("Error while creating data space (file) for field '%s'.", props.name);
- }
-
int rank;
hsize_t shape[2];
- hsize_t shape_total[2];
hsize_t offsets[2];
if (props.dimension > 1) {
rank = 2;
shape[0] = N;
shape[1] = props.dimension;
- shape_total[0] = N_total;
- shape_total[1] = props.dimension;
offsets[0] = offset;
offsets[1] = 0;
} else {
rank = 1;
shape[0] = N;
shape[1] = 0;
- shape_total[0] = N_total;
- shape_total[1] = 0;
offsets[0] = offset;
offsets[1] = 0;
}
@@ -293,34 +276,147 @@ void writeArray(struct engine* e, hid_t grp, char* fileName, FILE* xmfFile,
props.name);
}
+ /* Select the hyper-salb corresponding to this rank */
+ hid_t h_filespace = H5Dget_space(h_data);
+ if (N > 0) {
+ H5Sselect_hyperslab(h_filespace, H5S_SELECT_SET, offsets, NULL, shape,
+ NULL);
+ } else {
+ H5Sselect_none(h_filespace);
+ }
+
+ /* message("Writing %lld '%s', %zd elements = %zd bytes (int=%d) at offset
+ * %zd", */
+ /* N, props.name, N * props.dimension, N * props.dimension * typeSize, */
+ /* (int)(N * props.dimension * typeSize), offset); */
+
+ /* Write temporary buffer to HDF5 dataspace */
+ h_err = H5Dwrite(h_data, io_hdf5_type(props.type), h_memspace, h_filespace,
+ h_plist_id, temp);
+ if (h_err < 0) {
+ error("Error while writing data array '%s'.", props.name);
+ }
+
+ /* Free and close everything */
+ free(temp);
+ H5Sclose(h_memspace);
+ H5Sclose(h_filespace);
+}
+
+/**
+ * @brief Writes a data array in given HDF5 group.
+ *
+ * @param e The #engine we are writing from.
+ * @param grp The group in which to write.
+ * @param fileName The name of the file in which the data is written.
+ * @param xmfFile The FILE used to write the XMF description.
+ * @param partTypeGroupName The name of the group containing the particles in
+ * the HDF5 file.
+ * @param props The #io_props of the field to read
+ * @param N The number of particles to write.
+ * @param N_total Total number of particles across all cores.
+ * @param mpi_rank The rank of this node.
+ * @param offset Offset in the array where this mpi task starts writing.
+ * @param internal_units The #unit_system used internally.
+ * @param snapshot_units The #unit_system used in the snapshots.
+ */
+void writeArray(struct engine* e, hid_t grp, char* fileName, FILE* xmfFile,
+ char* partTypeGroupName, struct io_props props, size_t N,
+ long long N_total, int mpi_rank, long long offset,
+ const struct unit_system* internal_units,
+ const struct unit_system* snapshot_units) {
+
+ const size_t typeSize = io_sizeof_type(props.type);
+
+ /* Work out properties of the array in the file */
+ int rank;
+ hsize_t shape_total[2];
+ hsize_t chunk_shape[2];
+ if (props.dimension > 1) {
+ rank = 2;
+ shape_total[0] = N_total;
+ shape_total[1] = props.dimension;
+ chunk_shape[0] = 1 << 16; /* Just a guess...*/
+ chunk_shape[1] = props.dimension;
+ } else {
+ rank = 1;
+ shape_total[0] = N_total;
+ shape_total[1] = 0;
+ chunk_shape[0] = 1 << 16; /* Just a guess...*/
+ chunk_shape[1] = 0;
+ }
+
+ /* Make sure the chunks are not larger than the dataset */
+ if (chunk_shape[0] > (hsize_t)N_total) chunk_shape[0] = N_total;
+
+ /* Create the space in the file */
+ hid_t h_filespace = H5Screate(H5S_SIMPLE);
+ if (h_filespace < 0) {
+ error("Error while creating data space (file) for field '%s'.", props.name);
+ }
+
/* Change shape of file data space */
- h_err = H5Sset_extent_simple(h_filespace, rank, shape_total, NULL);
+ hid_t h_err = H5Sset_extent_simple(h_filespace, rank, shape_total, NULL);
if (h_err < 0) {
error("Error while changing data space (file) shape for field '%s'.",
props.name);
}
+ /* Dataset properties */
+ const hid_t h_prop = H5Pcreate(H5P_DATASET_CREATE);
+
+ /* Set chunk size */
+ /* h_err = H5Pset_chunk(h_prop, rank, chunk_shape); */
+ /* if (h_err < 0) { */
+ /* error("Error while setting chunk size (%llu, %llu) for field '%s'.", */
+ /* chunk_shape[0], chunk_shape[1], props.name); */
+ /* } */
+
/* Create dataset */
- const hid_t h_data =
- H5Dcreate(grp, props.name, io_hdf5_type(props.type), h_filespace,
- H5P_DEFAULT, H5P_DEFAULT, H5P_DEFAULT);
+ const hid_t h_data = H5Dcreate(grp, props.name, io_hdf5_type(props.type),
+ h_filespace, H5P_DEFAULT, h_prop, H5P_DEFAULT);
if (h_data < 0) {
error("Error while creating dataset '%s'.", props.name);
}
H5Sclose(h_filespace);
- h_filespace = H5Dget_space(h_data);
- H5Sselect_hyperslab(h_filespace, H5S_SELECT_SET, offsets, NULL, shape, NULL);
/* Create property list for collective dataset write. */
const hid_t h_plist_id = H5Pcreate(H5P_DATASET_XFER);
H5Pset_dxpl_mpio(h_plist_id, H5FD_MPIO_COLLECTIVE);
- /* Write temporary buffer to HDF5 dataspace */
- h_err = H5Dwrite(h_data, io_hdf5_type(props.type), h_memspace, h_filespace,
- h_plist_id, temp);
- if (h_err < 0) {
- error("Error while writing data array '%s'.", props.name);
+ /* Given the limitations of ROM-IO we will need to write the data in chunk of
+ HDF5_PARALLEL_IO_MAX_BYTES bytes per node until all the nodes are done. */
+ char redo = 1;
+ while (redo) {
+
+ /* Maximal number of elements */
+ const size_t max_chunk_size =
+ HDF5_PARALLEL_IO_MAX_BYTES / (props.dimension * typeSize);
+
+ /* Write the first chunk */
+ const size_t this_chunk = (N > max_chunk_size) ? max_chunk_size : N;
+ writeArray_chunk(e, h_data, h_plist_id, props, this_chunk, offset,
+ internal_units, snapshot_units);
+
+ /* Compute how many items are left */
+ if (N > max_chunk_size) {
+ N -= max_chunk_size;
+ props.field += max_chunk_size * props.partSize;
+ offset += max_chunk_size;
+ redo = 1;
+ } else {
+ N = 0;
+ offset += 0;
+ redo = 0;
+ }
+
+ /* Do we need to run again ? */
+ MPI_Allreduce(MPI_IN_PLACE, &redo, 1, MPI_SIGNED_CHAR, MPI_MAX,
+ MPI_COMM_WORLD);
+
+ if (redo && e->verbose && mpi_rank == 0)
+ message("Need to redo one iteration for array '%s'", props.name);
}
/* Write XMF description for this data set */
@@ -340,12 +436,10 @@ void writeArray(struct engine* e, hid_t grp, char* fileName, FILE* xmfFile,
units_a_factor(snapshot_units, props.units));
io_write_attribute_s(h_data, "Conversion factor", buffer);
- /* Free and close everything */
- free(temp);
+ /* Close everything */
+ H5Pclose(h_prop);
H5Dclose(h_data);
H5Pclose(h_plist_id);
- H5Sclose(h_memspace);
- H5Sclose(h_filespace);
}
/**
@@ -355,25 +449,23 @@ void writeArray(struct engine* e, hid_t grp, char* fileName, FILE* xmfFile,
* @param internal_units The system units used internally
* @param dim (output) The dimension of the volume read from the file.
* @param parts (output) The array of #part read from the file.
- * @param N (output) The number of particles read from the file.
+ * @param gparts (output) The array of #gpart read from the file.
+ * @param sparts (output) The array of #spart read from the file.
+ * @param Ngas (output) The number of particles read from the file.
+ * @param Ngparts (output) The number of particles read from the file.
+ * @param Nstars (output) The number of particles read from the file.
* @param periodic (output) 1 if the volume is periodic, 0 if not.
* @param flag_entropy (output) 1 if the ICs contained Entropy in the
* InternalEnergy field
+ * @param with_hydro Are we running with hydro ?
+ * @param with_gravity Are we running with gravity ?
+ * @param with_stars Are we running with stars ?
* @param mpi_rank The MPI rank of this node
* @param mpi_size The number of MPI ranks
* @param comm The MPI communicator
* @param info The MPI information object
* @param dry_run If 1, don't read the particle. Only allocates the arrays.
*
- * Opens the HDF5 file fileName and reads the particles contained
- * in the parts array. N is the returned number of particles found
- * in the file.
- *
- * @warning Can not read snapshot distributed over more than 1 file !!!
- * @todo Read snapshots distributed in more than one file.
- *
- * Calls #error() if an error occurs.
- *
*/
void read_ic_parallel(char* fileName, const struct unit_system* internal_units,
double dim[3], struct part** parts, struct gpart** gparts,
diff --git a/src/partition.c b/src/partition.c
index f30e5d0ad3c9ce8750a39891b2527729d9ad3b5d..1df369b18a635db1a3fef702306e69d663581d07 100644
--- a/src/partition.c
+++ b/src/partition.c
@@ -383,9 +383,8 @@ static void pick_metis(struct space *s, int nregions, int *vertexw, int *edgew,
/* dumpMETISGraph("metis_graph", idx_ncells, one, xadj, adjncy,
* weights_v, NULL, weights_e);
*/
-
- if (METIS_PartGraphKway(&idx_ncells, &one, xadj, adjncy, weights_v, weights_e,
- NULL, &idx_nregions, NULL, NULL, options, &objval,
+ if (METIS_PartGraphKway(&idx_ncells, &one, xadj, adjncy, weights_v, NULL,
+ weights_e, &idx_nregions, NULL, NULL, options, &objval,
regionid) != METIS_OK)
error("Call to METIS_PartGraphKway failed.");
@@ -520,11 +519,7 @@ static void repart_edge_metis(int partweights, int bothweights, int nodeID,
struct task *t = &tasks[j];
/* Skip un-interesting tasks. */
- if (t->type != task_type_self && t->type != task_type_pair &&
- t->type != task_type_sub_self && t->type != task_type_sub_self &&
- t->type != task_type_ghost && t->type != task_type_kick1 &&
- t->type != task_type_kick2 && t->type != task_type_timestep &&
- t->type != task_type_drift_part && t->type != task_type_drift_gpart)
+ if (t->cost == 0)
continue;
/* Get the task weight. */
diff --git a/src/runner.c b/src/runner.c
index b7ebf652738948141f8f3983b56331bad20e5a9d..73d7b5517fa073bef8e6fc3764733c7ec3e1f732 100644
--- a/src/runner.c
+++ b/src/runner.c
@@ -1885,7 +1885,7 @@ void *runner_main(void *data) {
runner_dopair1_branch_gradient(r, ci, cj);
#endif
else if (t->subtype == task_subtype_force)
- runner_dopair2_force(r, ci, cj);
+ runner_dopair2_branch_force(r, ci, cj);
else if (t->subtype == task_subtype_grav)
runner_dopair_grav(r, ci, cj, 1);
else
diff --git a/src/runner_doiact.h b/src/runner_doiact.h
index 3ea935b950a3989fbb79499a81a54f1bf8aca432..0d642b23c46aee7d31b9b3469afcca1a1041dbc6 100644
--- a/src/runner_doiact.h
+++ b/src/runner_doiact.h
@@ -32,6 +32,9 @@
#define _DOPAIR1(f) PASTE(runner_dopair1, f)
#define DOPAIR1 _DOPAIR1(FUNCTION)
+#define _DOPAIR2_BRANCH(f) PASTE(runner_dopair2_branch, f)
+#define DOPAIR2_BRANCH _DOPAIR2_BRANCH(FUNCTION)
+
#define _DOPAIR2(f) PASTE(runner_dopair2, f)
#define DOPAIR2 _DOPAIR2(FUNCTION)
@@ -778,37 +781,6 @@ void DOPAIR1(struct runner *r, struct cell *ci, struct cell *cj, const int sid,
const struct entry *restrict sort_j = cj->sort[sid];
#ifdef SWIFT_DEBUG_CHECKS
- /* Check that the dx_max_sort values in the cell are indeed an upper
- bound on particle movement. */
- for (int pid = 0; pid < ci->count; pid++) {
- const struct part *p = &ci->parts[sort_i[pid].i];
- const float d = p->x[0] * runner_shift[sid][0] +
- p->x[1] * runner_shift[sid][1] +
- p->x[2] * runner_shift[sid][2];
- if (fabsf(d - sort_i[pid].d) - ci->dx_max_sort >
- 1.0e-4 * max(fabsf(d), ci->dx_max_sort_old))
- error(
- "particle shift diff exceeds dx_max_sort in cell ci. ci->nodeID=%d "
- "cj->nodeID=%d d=%e sort_i[pid].d=%e ci->dx_max_sort=%e "
- "ci->dx_max_sort_old=%e",
- ci->nodeID, cj->nodeID, d, sort_i[pid].d, ci->dx_max_sort,
- ci->dx_max_sort_old);
- }
- for (int pjd = 0; pjd < cj->count; pjd++) {
- const struct part *p = &cj->parts[sort_j[pjd].i];
- const float d = p->x[0] * runner_shift[sid][0] +
- p->x[1] * runner_shift[sid][1] +
- p->x[2] * runner_shift[sid][2];
- if (fabsf(d - sort_j[pjd].d) - cj->dx_max_sort >
- 1.0e-4 * max(fabsf(d), cj->dx_max_sort_old))
- error(
- "particle shift diff exceeds dx_max_sort in cell cj. cj->nodeID=%d "
- "ci->nodeID=%d d=%e sort_j[pjd].d=%e cj->dx_max_sort=%e "
- "cj->dx_max_sort_old=%e",
- cj->nodeID, ci->nodeID, d, sort_j[pjd].d, cj->dx_max_sort,
- cj->dx_max_sort_old);
- }
-
/* Some constants used to checks that the parts are in the right frame */
const float shift_threshold_x =
2. * ci->width[0] + 2. * max(ci->dx_max_part, cj->dx_max_part);
@@ -816,7 +788,6 @@ void DOPAIR1(struct runner *r, struct cell *ci, struct cell *cj, const int sid,
2. * ci->width[1] + 2. * max(ci->dx_max_part, cj->dx_max_part);
const float shift_threshold_z =
2. * ci->width[2] + 2. * max(ci->dx_max_part, cj->dx_max_part);
-
#endif /* SWIFT_DEBUG_CHECKS */
/* Get some other useful values. */
@@ -1025,6 +996,43 @@ void DOPAIR1_BRANCH(struct runner *r, struct cell *ci, struct cell *cj) {
cj->dx_max_sort_old > space_maxreldx * cj->dmin)
error("Interacting unsorted cells.");
+#ifdef SWIFT_DEBUG_CHECKS
+ /* Pick-out the sorted lists. */
+ const struct entry *restrict sort_i = ci->sort[sid];
+ const struct entry *restrict sort_j = cj->sort[sid];
+
+ /* Check that the dx_max_sort values in the cell are indeed an upper
+ bound on particle movement. */
+ for (int pid = 0; pid < ci->count; pid++) {
+ const struct part *p = &ci->parts[sort_i[pid].i];
+ const float d = p->x[0] * runner_shift[sid][0] +
+ p->x[1] * runner_shift[sid][1] +
+ p->x[2] * runner_shift[sid][2];
+ if (fabsf(d - sort_i[pid].d) - ci->dx_max_sort >
+ 1.0e-4 * max(fabsf(d), ci->dx_max_sort_old))
+ error(
+ "particle shift diff exceeds dx_max_sort in cell ci. ci->nodeID=%d "
+ "cj->nodeID=%d d=%e sort_i[pid].d=%e ci->dx_max_sort=%e "
+ "ci->dx_max_sort_old=%e",
+ ci->nodeID, cj->nodeID, d, sort_i[pid].d, ci->dx_max_sort,
+ ci->dx_max_sort_old);
+ }
+ for (int pjd = 0; pjd < cj->count; pjd++) {
+ const struct part *p = &cj->parts[sort_j[pjd].i];
+ const float d = p->x[0] * runner_shift[sid][0] +
+ p->x[1] * runner_shift[sid][1] +
+ p->x[2] * runner_shift[sid][2];
+ if (fabsf(d - sort_j[pjd].d) - cj->dx_max_sort >
+ 1.0e-4 * max(fabsf(d), cj->dx_max_sort_old))
+ error(
+ "particle shift diff exceeds dx_max_sort in cell cj. cj->nodeID=%d "
+ "ci->nodeID=%d d=%e sort_j[pjd].d=%e cj->dx_max_sort=%e "
+ "cj->dx_max_sort_old=%e",
+ cj->nodeID, ci->nodeID, d, sort_j[pjd].d, cj->dx_max_sort,
+ cj->dx_max_sort_old);
+ }
+#endif /* SWIFT_DEBUG_CHECKS */
+
#if defined(WITH_VECTORIZATION) && defined(GADGET2_SPH) && \
(DOPAIR1_BRANCH == runner_dopair1_density_branch)
if (!sort_is_corner(sid))
@@ -1042,8 +1050,11 @@ void DOPAIR1_BRANCH(struct runner *r, struct cell *ci, struct cell *cj) {
* @param r The #runner.
* @param ci The first #cell.
* @param cj The second #cell.
+ * @param sid The direction of the pair
+ * @param shift The shift vector to apply to the particles in ci.
*/
-void DOPAIR2(struct runner *r, struct cell *ci, struct cell *cj) {
+void DOPAIR2(struct runner *r, struct cell *ci, struct cell *cj, const int sid,
+ const double *shift) {
struct engine *restrict e = r->e;
@@ -1054,24 +1065,6 @@ void DOPAIR2(struct runner *r, struct cell *ci, struct cell *cj) {
TIMER_TIC;
- /* Anything to do here? */
- if (!cell_is_active(ci, e) && !cell_is_active(cj, e)) return;
-
- if (!cell_are_part_drifted(ci, e) || !cell_are_part_drifted(cj, e))
- error("Interacting undrifted cells.");
-
- /* Get the shift ID. */
- double shift[3] = {0.0, 0.0, 0.0};
- const int sid = space_getsid(e->s, &ci, &cj, shift);
-
- /* Have the cells been sorted? */
- if (!(ci->sorted & (1 << sid)) ||
- ci->dx_max_sort_old > space_maxreldx * ci->dmin)
- error("Interacting unsorted cells.");
- if (!(cj->sorted & (1 << sid)) ||
- cj->dx_max_sort_old > space_maxreldx * cj->dmin)
- error("Interacting unsorted cells.");
-
/* Get the cutoff shift. */
double rshift = 0.0;
for (int k = 0; k < 3; k++) rshift += shift[k] * runner_shift[sid][k];
@@ -1081,37 +1074,6 @@ void DOPAIR2(struct runner *r, struct cell *ci, struct cell *cj) {
struct entry *restrict sort_j = cj->sort[sid];
#ifdef SWIFT_DEBUG_CHECKS
- /* Check that the dx_max_sort values in the cell are indeed an upper
- bound on particle movement. */
- for (int pid = 0; pid < ci->count; pid++) {
- const struct part *p = &ci->parts[sort_i[pid].i];
- const float d = p->x[0] * runner_shift[sid][0] +
- p->x[1] * runner_shift[sid][1] +
- p->x[2] * runner_shift[sid][2];
- if (fabsf(d - sort_i[pid].d) - ci->dx_max_sort >
- 1.0e-4 * max(fabsf(d), ci->dx_max_sort_old))
- error(
- "particle shift diff exceeds dx_max_sort in cell ci. ci->nodeID=%d "
- "cj->nodeID=%d d=%e sort_i[pid].d=%e ci->dx_max_sort=%e "
- "ci->dx_max_sort_old=%e",
- ci->nodeID, cj->nodeID, d, sort_i[pid].d, ci->dx_max_sort,
- ci->dx_max_sort_old);
- }
- for (int pjd = 0; pjd < cj->count; pjd++) {
- const struct part *p = &cj->parts[sort_j[pjd].i];
- const float d = p->x[0] * runner_shift[sid][0] +
- p->x[1] * runner_shift[sid][1] +
- p->x[2] * runner_shift[sid][2];
- if (fabsf(d - sort_j[pjd].d) - cj->dx_max_sort >
- 1.0e-4 * max(fabsf(d), cj->dx_max_sort_old))
- error(
- "particle shift diff exceeds dx_max_sort in cell cj. cj->nodeID=%d "
- "ci->nodeID=%d d=%e sort_j[pjd].d=%e cj->dx_max_sort=%e "
- "cj->dx_max_sort_old=%e",
- cj->nodeID, ci->nodeID, d, sort_j[pjd].d, cj->dx_max_sort,
- cj->dx_max_sort_old);
- }
-
/* Some constants used to checks that the parts are in the right frame */
const float shift_threshold_x =
2. * ci->width[0] + 2. * max(ci->dx_max_part, cj->dx_max_part);
@@ -1119,7 +1081,6 @@ void DOPAIR2(struct runner *r, struct cell *ci, struct cell *cj) {
2. * ci->width[1] + 2. * max(ci->dx_max_part, cj->dx_max_part);
const float shift_threshold_z =
2. * ci->width[2] + 2. * max(ci->dx_max_part, cj->dx_max_part);
-
#endif /* SWIFT_DEBUG_CHECKS */
/* Get some other useful values. */
@@ -1490,6 +1451,86 @@ void DOPAIR2(struct runner *r, struct cell *ci, struct cell *cj) {
TIMER_TOC(TIMER_DOPAIR);
}
+/**
+ * @brief Determine which version of DOPAIR2 needs to be called depending on the
+ * orientation of the cells or whether DOPAIR2 needs to be called at all.
+ *
+ * @param r #runner
+ * @param ci #cell ci
+ * @param cj #cell cj
+ *
+ */
+void DOPAIR2_BRANCH(struct runner *r, struct cell *ci, struct cell *cj) {
+
+ const struct engine *restrict e = r->e;
+
+ /* Anything to do here? */
+ if (!cell_is_active(ci, e) && !cell_is_active(cj, e)) return;
+
+ /* Check that cells are drifted. */
+ if (!cell_are_part_drifted(ci, e) || !cell_are_part_drifted(cj, e))
+ error("Interacting undrifted cells.");
+
+ /* Get the sort ID. */
+ double shift[3] = {0.0, 0.0, 0.0};
+ const int sid = space_getsid(e->s, &ci, &cj, shift);
+
+ /* Have the cells been sorted? */
+ if (!(ci->sorted & (1 << sid)) ||
+ ci->dx_max_sort_old > space_maxreldx * ci->dmin)
+ error("Interacting unsorted cells.");
+ if (!(cj->sorted & (1 << sid)) ||
+ cj->dx_max_sort_old > space_maxreldx * cj->dmin)
+ error("Interacting unsorted cells.");
+
+#ifdef SWIFT_DEBUG_CHECKS
+ /* Pick-out the sorted lists. */
+ const struct entry *restrict sort_i = ci->sort[sid];
+ const struct entry *restrict sort_j = cj->sort[sid];
+
+ /* Check that the dx_max_sort values in the cell are indeed an upper
+ bound on particle movement. */
+ for (int pid = 0; pid < ci->count; pid++) {
+ const struct part *p = &ci->parts[sort_i[pid].i];
+ const float d = p->x[0] * runner_shift[sid][0] +
+ p->x[1] * runner_shift[sid][1] +
+ p->x[2] * runner_shift[sid][2];
+ if (fabsf(d - sort_i[pid].d) - ci->dx_max_sort >
+ 1.0e-4 * max(fabsf(d), ci->dx_max_sort_old))
+ error(
+ "particle shift diff exceeds dx_max_sort in cell ci. ci->nodeID=%d "
+ "cj->nodeID=%d d=%e sort_i[pid].d=%e ci->dx_max_sort=%e "
+ "ci->dx_max_sort_old=%e",
+ ci->nodeID, cj->nodeID, d, sort_i[pid].d, ci->dx_max_sort,
+ ci->dx_max_sort_old);
+ }
+ for (int pjd = 0; pjd < cj->count; pjd++) {
+ const struct part *p = &cj->parts[sort_j[pjd].i];
+ const float d = p->x[0] * runner_shift[sid][0] +
+ p->x[1] * runner_shift[sid][1] +
+ p->x[2] * runner_shift[sid][2];
+ if (fabsf(d - sort_j[pjd].d) - cj->dx_max_sort >
+ 1.0e-4 * max(fabsf(d), cj->dx_max_sort_old))
+ error(
+ "particle shift diff exceeds dx_max_sort in cell cj. cj->nodeID=%d "
+ "ci->nodeID=%d d=%e sort_j[pjd].d=%e cj->dx_max_sort=%e "
+ "cj->dx_max_sort_old=%e",
+ cj->nodeID, ci->nodeID, d, sort_j[pjd].d, cj->dx_max_sort,
+ cj->dx_max_sort_old);
+ }
+#endif /* SWIFT_DEBUG_CHECKS */
+
+#if defined(WITH_VECTORIZATION) && defined(GADGET2_SPH) && \
+ (DOPAIR2_BRANCH == runner_dopair2_force_branch)
+ if (!sort_is_corner(sid))
+ runner_dopair2_force_vec(r, ci, cj, sid, shift);
+ else
+ DOPAIR2(r, ci, cj, sid, shift);
+#else
+ DOPAIR2(r, ci, cj, sid, shift);
+#endif
+}
+
/**
* @brief Compute the cell self-interaction (non-symmetric).
*
@@ -2295,7 +2336,7 @@ void DOSUB_PAIR2(struct runner *r, struct cell *ci, struct cell *cj, int sid,
error("Interacting unsorted cells.");
/* Compute the interactions. */
- DOPAIR2(r, ci, cj);
+ DOPAIR2_BRANCH(r, ci, cj);
}
if (gettimer) TIMER_TOC(TIMER_DOSUB_PAIR);
diff --git a/src/runner_doiact_vec.c b/src/runner_doiact_vec.c
index 5e982830c609bcf2ce533c0423449a3e74e96bf4..7e34939ac4e6741dc9fd970f774bba01ca812593 100644
--- a/src/runner_doiact_vec.c
+++ b/src/runner_doiact_vec.c
@@ -35,21 +35,23 @@ static const vector kernel_gamma2_vec = FILL_VEC(kernel_gamma2);
* @param int_cache (return) secondary #cache of interactions between two
* particles.
* @param icount Interaction count.
- * @param rhoSum (return) #vector holding the cumulative sum of the density
+ * @param v_rhoSum (return) #vector holding the cumulative sum of the density
* update on pi.
- * @param rho_dhSum (return) #vector holding the cumulative sum of the density
+ * @param v_rho_dhSum (return) #vector holding the cumulative sum of the density
* gradient update on pi.
- * @param wcountSum (return) #vector holding the cumulative sum of the wcount
+ * @param v_wcountSum (return) #vector holding the cumulative sum of the wcount
* update on pi.
- * @param wcount_dhSum (return) #vector holding the cumulative sum of the wcount
+ * @param v_wcount_dhSum (return) #vector holding the cumulative sum of the
+ * wcount
* gradient update on pi.
- * @param div_vSum (return) #vector holding the cumulative sum of the divergence
+ * @param v_div_vSum (return) #vector holding the cumulative sum of the
+ * divergence
* update on pi.
- * @param curlvxSum (return) #vector holding the cumulative sum of the curl of
+ * @param v_curlvxSum (return) #vector holding the cumulative sum of the curl of
* vx update on pi.
- * @param curlvySum (return) #vector holding the cumulative sum of the curl of
+ * @param v_curlvySum (return) #vector holding the cumulative sum of the curl of
* vy update on pi.
- * @param curlvzSum (return) #vector holding the cumulative sum of the curl of
+ * @param v_curlvzSum (return) #vector holding the cumulative sum of the curl of
* vz update on pi.
* @param v_hi_inv #vector of 1/h for pi.
* @param v_vix #vector of x velocity of pi.
@@ -59,11 +61,11 @@ static const vector kernel_gamma2_vec = FILL_VEC(kernel_gamma2);
* interactions have been performed, should be a multiple of the vector length.
*/
__attribute__((always_inline)) INLINE static void calcRemInteractions(
- struct c2_cache *const int_cache, const int icount, vector *rhoSum,
- vector *rho_dhSum, vector *wcountSum, vector *wcount_dhSum,
- vector *div_vSum, vector *curlvxSum, vector *curlvySum, vector *curlvzSum,
- vector v_hi_inv, vector v_vix, vector v_viy, vector v_viz,
- int *icount_align) {
+ struct c2_cache *const int_cache, const int icount, vector *v_rhoSum,
+ vector *v_rho_dhSum, vector *v_wcountSum, vector *v_wcount_dhSum,
+ vector *v_div_vSum, vector *v_curlvxSum, vector *v_curlvySum,
+ vector *v_curlvzSum, vector v_hi_inv, vector v_vix, vector v_viy,
+ vector v_viz, int *icount_align) {
mask_t int_mask, int_mask2;
@@ -107,9 +109,9 @@ __attribute__((always_inline)) INLINE static void calcRemInteractions(
&int_cache->dyq[*icount_align], &int_cache->dzq[*icount_align],
v_hi_inv, v_vix, v_viy, v_viz, &int_cache->vxq[*icount_align],
&int_cache->vyq[*icount_align], &int_cache->vzq[*icount_align],
- &int_cache->mq[*icount_align], rhoSum, rho_dhSum, wcountSum,
- wcount_dhSum, div_vSum, curlvxSum, curlvySum, curlvzSum, int_mask,
- int_mask2, 1);
+ &int_cache->mq[*icount_align], v_rhoSum, v_rho_dhSum, v_wcountSum,
+ v_wcount_dhSum, v_div_vSum, v_curlvxSum, v_curlvySum, v_curlvzSum,
+ int_mask, int_mask2, 1);
}
}
@@ -127,20 +129,25 @@ __attribute__((always_inline)) INLINE static void calcRemInteractions(
* @param int_cache (return) secondary #cache of interactions between two
* particles.
* @param icount Interaction count.
- * @param rhoSum #vector holding the cumulative sum of the density update on pi.
- * @param rho_dhSum #vector holding the cumulative sum of the density gradient
+ * @param v_rhoSum #vector holding the cumulative sum of the density update on
+ * pi.
+ * @param v_rho_dhSum #vector holding the cumulative sum of the density gradient
* update on pi.
- * @param wcountSum #vector holding the cumulative sum of the wcount update on
+ * @param v_wcountSum #vector holding the cumulative sum of the wcount update on
* pi.
- * @param wcount_dhSum #vector holding the cumulative sum of the wcount gradient
+ * @param v_wcount_dhSum #vector holding the cumulative sum of the wcount
+ * gradient
* update on pi.
- * @param div_vSum #vector holding the cumulative sum of the divergence update
+ * @param v_div_vSum #vector holding the cumulative sum of the divergence update
* on pi.
- * @param curlvxSum #vector holding the cumulative sum of the curl of vx update
+ * @param v_curlvxSum #vector holding the cumulative sum of the curl of vx
+ * update
* on pi.
- * @param curlvySum #vector holding the cumulative sum of the curl of vy update
+ * @param v_curlvySum #vector holding the cumulative sum of the curl of vy
+ * update
* on pi.
- * @param curlvzSum #vector holding the cumulative sum of the curl of vz update
+ * @param v_curlvzSum #vector holding the cumulative sum of the curl of vz
+ * update
* on pi.
* @param v_hi_inv #vector of 1/h for pi.
* @param v_vix #vector of x velocity of pi.
@@ -150,10 +157,11 @@ __attribute__((always_inline)) INLINE static void calcRemInteractions(
__attribute__((always_inline)) INLINE static void storeInteractions(
const int mask, const int pjd, vector *v_r2, vector *v_dx, vector *v_dy,
vector *v_dz, const struct cache *const cell_cache,
- struct c2_cache *const int_cache, int *icount, vector *rhoSum,
- vector *rho_dhSum, vector *wcountSum, vector *wcount_dhSum,
- vector *div_vSum, vector *curlvxSum, vector *curlvySum, vector *curlvzSum,
- vector v_hi_inv, vector v_vix, vector v_viy, vector v_viz) {
+ struct c2_cache *const int_cache, int *icount, vector *v_rhoSum,
+ vector *v_rho_dhSum, vector *v_wcountSum, vector *v_wcount_dhSum,
+ vector *v_div_vSum, vector *v_curlvxSum, vector *v_curlvySum,
+ vector *v_curlvzSum, vector v_hi_inv, vector v_vix, vector v_viy,
+ vector v_viz) {
/* Left-pack values needed into the secondary cache using the interaction mask.
*/
@@ -202,9 +210,10 @@ __attribute__((always_inline)) INLINE static void storeInteractions(
int icount_align = *icount;
/* Peform remainder interactions. */
- calcRemInteractions(int_cache, *icount, rhoSum, rho_dhSum, wcountSum,
- wcount_dhSum, div_vSum, curlvxSum, curlvySum, curlvzSum,
- v_hi_inv, v_vix, v_viy, v_viz, &icount_align);
+ calcRemInteractions(int_cache, *icount, v_rhoSum, v_rho_dhSum, v_wcountSum,
+ v_wcount_dhSum, v_div_vSum, v_curlvxSum, v_curlvySum,
+ v_curlvzSum, v_hi_inv, v_vix, v_viy, v_viz,
+ &icount_align);
mask_t int_mask, int_mask2;
vec_init_mask_true(int_mask);
@@ -215,9 +224,9 @@ __attribute__((always_inline)) INLINE static void storeInteractions(
runner_iact_nonsym_2_vec_density(
&int_cache->r2q[j], &int_cache->dxq[j], &int_cache->dyq[j],
&int_cache->dzq[j], v_hi_inv, v_vix, v_viy, v_viz, &int_cache->vxq[j],
- &int_cache->vyq[j], &int_cache->vzq[j], &int_cache->mq[j], rhoSum,
- rho_dhSum, wcountSum, wcount_dhSum, div_vSum, curlvxSum, curlvySum,
- curlvzSum, int_mask, int_mask2, 0);
+ &int_cache->vyq[j], &int_cache->vzq[j], &int_cache->mq[j], v_rhoSum,
+ v_rho_dhSum, v_wcountSum, v_wcount_dhSum, v_div_vSum, v_curlvxSum,
+ v_curlvySum, v_curlvzSum, int_mask, int_mask2, 0);
}
/* Reset interaction count. */
@@ -288,8 +297,9 @@ __attribute__((always_inline)) INLINE static void populate_max_index_no_cache(
const float first_di =
sort_i[first_pi].d + pi->h * kernel_gamma + dx_max - rshift;
- /* Loop through particles in cell j until they are not in range of pi. */
- while (temp < cj->count && first_di > sort_j[temp].d) temp++;
+ /* Loop through particles in cell j until they are not in range of pi.
+ * Make sure that temp stays between 0 and cj->count - 1.*/
+ while (temp < cj->count - 1 && first_di > sort_j[temp].d) temp++;
max_index_i[first_pi] = temp;
@@ -300,7 +310,8 @@ __attribute__((always_inline)) INLINE static void populate_max_index_no_cache(
const float di = sort_i[i].d + pi->h * kernel_gamma + dx_max - rshift;
- while (temp < cj->count && di > sort_j[temp].d) temp++;
+ /* Make sure that temp stays between 0 and cj->count - 1.*/
+ while (temp < cj->count - 1 && di > sort_j[temp].d) temp++;
max_index_i[i] = temp;
}
@@ -357,6 +368,153 @@ __attribute__((always_inline)) INLINE static void populate_max_index_no_cache(
*init_pi = first_pi;
*init_pj = last_pj;
}
+
+/**
+ * @brief Populates the arrays max_index_i and max_index_j with the maximum
+ * indices of
+ * particles into their neighbouring cells. Also finds the first pi that
+ * interacts with any particle in cj and the last pj that interacts with any
+ * particle in ci.
+ *
+ * @param ci #cell pointer to ci
+ * @param cj #cell pointer to cj
+ * @param sort_i #entry array for particle distance in ci
+ * @param sort_j #entry array for particle distance in cj
+ * @param dx_max maximum particle movement allowed in cell
+ * @param rshift cutoff shift
+ * @param hi_max_raw Maximal smoothing length in cell ci
+ * @param hj_max_raw Maximal smoothing length in cell cj
+ * @param hi_max Maximal smoothing length in cell ci scaled by kernel_gamma
+ * @param hj_max Maximal smoothing length in cell cj scaled by kernel_gamma
+ * @param di_max Maximal position on the axis that can interact in cell ci
+ * @param dj_min Minimal position on the axis that can interact in cell ci
+ * @param max_index_i array to hold the maximum distances of pi particles into
+ * #cell cj
+ * @param max_index_j array to hold the maximum distances of pj particles into
+ * #cell cj
+ * @param init_pi first pi to interact with a pj particle
+ * @param init_pj last pj to interact with a pi particle
+ * @param max_active_bin The largest time-bin active during this step.
+ */
+__attribute__((always_inline)) INLINE static void
+populate_max_index_no_cache_force(const struct cell *ci, const struct cell *cj,
+ const struct entry *restrict sort_i,
+ const struct entry *restrict sort_j,
+ const float dx_max, const float rshift,
+ const double hi_max_raw,
+ const double hj_max_raw, const double hi_max,
+ const double hj_max, const double di_max,
+ const double dj_min, int *max_index_i,
+ int *max_index_j, int *init_pi, int *init_pj,
+ const timebin_t max_active_bin) {
+
+ const struct part *restrict parts_i = ci->parts;
+ const struct part *restrict parts_j = cj->parts;
+
+ int first_pi = 0, last_pj = cj->count - 1;
+ int temp;
+
+ /* Find the leftmost active particle in cell i that interacts with any
+ * particle in cell j. */
+ first_pi = ci->count;
+ int active_id = first_pi - 1;
+ while (first_pi > 0 &&
+ sort_i[first_pi - 1].d + dx_max + max(hi_max, hj_max) > dj_min) {
+ first_pi--;
+ /* Store the index of the particle if it is active. */
+ if (part_is_active_no_debug(&parts_i[sort_i[first_pi].i], max_active_bin))
+ active_id = first_pi;
+ }
+
+ /* Set the first active pi in range of any particle in cell j. */
+ first_pi = active_id;
+
+ /* Find the maximum index into cell j for each particle in range in cell i. */
+ if (first_pi < ci->count) {
+
+ /* Start from the first particle in cell j. */
+ temp = 0;
+
+ const struct part *pi = &parts_i[sort_i[first_pi].i];
+ const float first_di = sort_i[first_pi].d +
+ max(pi->h, hj_max_raw) * kernel_gamma + dx_max -
+ rshift;
+
+ /* Loop through particles in cell j until they are not in range of pi.
+ * Make sure that temp stays between 0 and cj->count - 1.*/
+ while (temp < cj->count - 1 && first_di > sort_j[temp].d) temp++;
+
+ max_index_i[first_pi] = temp;
+
+ /* Populate max_index_i for remaining particles that are within range. */
+ for (int i = first_pi + 1; i < ci->count; i++) {
+ temp = max_index_i[i - 1];
+ pi = &parts_i[sort_i[i].i];
+
+ const float di =
+ sort_i[i].d + max(pi->h, hj_max_raw) * kernel_gamma + dx_max - rshift;
+
+ /* Make sure that temp stays between 0 and cj->count - 1.*/
+ while (temp < cj->count - 1 && di > sort_j[temp].d) temp++;
+
+ max_index_i[i] = temp;
+ }
+ } else {
+ /* Make sure that max index is set to first particle in cj.*/
+ max_index_i[ci->count - 1] = 0;
+ }
+
+ /* Find the rightmost active particle in cell j that interacts with any
+ * particle in cell i. */
+ last_pj = -1;
+ active_id = last_pj;
+ while (last_pj < cj->count &&
+ sort_j[last_pj + 1].d - max(hj_max, hi_max) - dx_max < di_max) {
+ last_pj++;
+ /* Store the index of the particle if it is active. */
+ if (part_is_active_no_debug(&parts_j[sort_j[last_pj].i], max_active_bin))
+ active_id = last_pj;
+ }
+
+ /* Set the last active pj in range of any particle in cell i. */
+ last_pj = active_id;
+
+ /* Find the maximum index into cell i for each particle in range in cell j. */
+ if (last_pj >= 0) {
+
+ /* Start from the last particle in cell i. */
+ temp = ci->count - 1;
+
+ const struct part *pj = &parts_j[sort_j[last_pj].i];
+ const float last_dj = sort_j[last_pj].d - dx_max -
+ max(pj->h, hi_max_raw) * kernel_gamma + rshift;
+
+ /* Loop through particles in cell i until they are not in range of pj. */
+ while (temp > 0 && last_dj < sort_i[temp].d) temp--;
+
+ max_index_j[last_pj] = temp;
+
+ /* Populate max_index_j for remaining particles that are within range. */
+ for (int i = last_pj - 1; i >= 0; i--) {
+ temp = max_index_j[i + 1];
+ pj = &parts_j[sort_j[i].i];
+
+ const float dj = sort_j[i].d - dx_max -
+ (max(pj->h, hi_max_raw) * kernel_gamma) + rshift;
+
+ while (temp > 0 && dj < sort_i[temp].d) temp--;
+
+ max_index_j[i] = temp;
+ }
+ } else {
+ /* Make sure that max index is set to last particle in ci.*/
+ max_index_j[0] = ci->count - 1;
+ }
+
+ *init_pi = first_pi;
+ *init_pj = last_pj;
+}
+
#endif /* WITH_VECTORIZATION */
/**
@@ -370,20 +528,17 @@ __attribute__((always_inline)) INLINE void runner_doself1_density_vec(
struct runner *r, struct cell *restrict c) {
#ifdef WITH_VECTORIZATION
- const struct engine *e = r->e;
- struct part *restrict pi;
- int count_align;
- int num_vec_proc = NUM_VEC_PROC;
+ const int num_vec_proc = NUM_VEC_PROC;
+ /* Get some local variables */
+ const struct engine *e = r->e;
+ const timebin_t max_active_bin = e->max_active_bin;
struct part *restrict parts = c->parts;
const int count = c->count;
- const timebin_t max_active_bin = e->max_active_bin;
-
- vector v_hi, v_vix, v_viy, v_viz, v_hig2, v_r2;
-
- TIMER_TIC
+ TIMER_TIC;
+ /* Anything to do here? */
if (!cell_is_active(c, e)) return;
if (!cell_are_part_drifted(c, e)) error("Interacting undrifted cell.");
@@ -407,88 +562,78 @@ __attribute__((always_inline)) INLINE void runner_doself1_density_vec(
for (int pid = 0; pid < count; pid++) {
/* Get a pointer to the ith particle. */
- pi = &parts[pid];
+ struct part *restrict pi = &parts[pid];
/* Is the ith particle active? */
if (!part_is_active_no_debug(pi, max_active_bin)) continue;
- vector pix, piy, piz;
+ vector v_r2;
const float hi = cell_cache->h[pid];
/* Fill particle pi vectors. */
- pix.v = vec_set1(cell_cache->x[pid]);
- piy.v = vec_set1(cell_cache->y[pid]);
- piz.v = vec_set1(cell_cache->z[pid]);
- v_hi.v = vec_set1(hi);
- v_vix.v = vec_set1(cell_cache->vx[pid]);
- v_viy.v = vec_set1(cell_cache->vy[pid]);
- v_viz.v = vec_set1(cell_cache->vz[pid]);
+ const vector v_pix = vector_set1(cell_cache->x[pid]);
+ const vector v_piy = vector_set1(cell_cache->y[pid]);
+ const vector v_piz = vector_set1(cell_cache->z[pid]);
+ const vector v_hi = vector_set1(hi);
+ const vector v_vix = vector_set1(cell_cache->vx[pid]);
+ const vector v_viy = vector_set1(cell_cache->vy[pid]);
+ const vector v_viz = vector_set1(cell_cache->vz[pid]);
const float hig2 = hi * hi * kernel_gamma2;
- v_hig2.v = vec_set1(hig2);
-
- /* Reset cumulative sums of update vectors. */
- vector rhoSum, rho_dhSum, wcountSum, wcount_dhSum, div_vSum, curlvxSum,
- curlvySum, curlvzSum;
+ const vector v_hig2 = vector_set1(hig2);
/* Get the inverse of hi. */
- vector v_hi_inv;
-
- v_hi_inv = vec_reciprocal(v_hi);
+ vector v_hi_inv = vec_reciprocal(v_hi);
- rhoSum.v = vec_setzero();
- rho_dhSum.v = vec_setzero();
- wcountSum.v = vec_setzero();
- wcount_dhSum.v = vec_setzero();
- div_vSum.v = vec_setzero();
- curlvxSum.v = vec_setzero();
- curlvySum.v = vec_setzero();
- curlvzSum.v = vec_setzero();
+ /* Reset cumulative sums of update vectors. */
+ vector v_rhoSum = vector_setzero();
+ vector v_rho_dhSum = vector_setzero();
+ vector v_wcountSum = vector_setzero();
+ vector v_wcount_dhSum = vector_setzero();
+ vector v_div_vSum = vector_setzero();
+ vector v_curlvxSum = vector_setzero();
+ vector v_curlvySum = vector_setzero();
+ vector v_curlvzSum = vector_setzero();
/* Pad cache if there is a serial remainder. */
- count_align = count;
- int rem = count % (num_vec_proc * VEC_SIZE);
+ int count_align = count;
+ const int rem = count % (num_vec_proc * VEC_SIZE);
if (rem != 0) {
- int pad = (num_vec_proc * VEC_SIZE) - rem;
-
- count_align += pad;
+ count_align += (num_vec_proc * VEC_SIZE) - rem;
/* Set positions to the same as particle pi so when the r2 > 0 mask is
* applied these extra contributions are masked out.*/
for (int i = count; i < count_align; i++) {
- cell_cache->x[i] = pix.f[0];
- cell_cache->y[i] = piy.f[0];
- cell_cache->z[i] = piz.f[0];
+ cell_cache->x[i] = v_pix.f[0];
+ cell_cache->y[i] = v_piy.f[0];
+ cell_cache->z[i] = v_piz.f[0];
}
}
- vector pjx, pjy, pjz;
- vector pjx2, pjy2, pjz2;
-
/* Find all of particle pi's interacions and store needed values in the
* secondary cache.*/
for (int pjd = 0; pjd < count_align; pjd += (num_vec_proc * VEC_SIZE)) {
/* Load 2 sets of vectors from the particle cache. */
- pjx.v = vec_load(&cell_cache->x[pjd]);
- pjy.v = vec_load(&cell_cache->y[pjd]);
- pjz.v = vec_load(&cell_cache->z[pjd]);
+ const vector v_pjx = vector_load(&cell_cache->x[pjd]);
+ const vector v_pjy = vector_load(&cell_cache->y[pjd]);
+ const vector v_pjz = vector_load(&cell_cache->z[pjd]);
- pjx2.v = vec_load(&cell_cache->x[pjd + VEC_SIZE]);
- pjy2.v = vec_load(&cell_cache->y[pjd + VEC_SIZE]);
- pjz2.v = vec_load(&cell_cache->z[pjd + VEC_SIZE]);
+ const vector v_pjx2 = vector_load(&cell_cache->x[pjd + VEC_SIZE]);
+ const vector v_pjy2 = vector_load(&cell_cache->y[pjd + VEC_SIZE]);
+ const vector v_pjz2 = vector_load(&cell_cache->z[pjd + VEC_SIZE]);
/* Compute the pairwise distance. */
vector v_dx, v_dy, v_dz;
vector v_dx_2, v_dy_2, v_dz_2, v_r2_2;
- v_dx.v = vec_sub(pix.v, pjx.v);
- v_dx_2.v = vec_sub(pix.v, pjx2.v);
- v_dy.v = vec_sub(piy.v, pjy.v);
- v_dy_2.v = vec_sub(piy.v, pjy2.v);
- v_dz.v = vec_sub(piz.v, pjz.v);
- v_dz_2.v = vec_sub(piz.v, pjz2.v);
+ v_dx.v = vec_sub(v_pix.v, v_pjx.v);
+ v_dx_2.v = vec_sub(v_pix.v, v_pjx2.v);
+ v_dy.v = vec_sub(v_piy.v, v_pjy.v);
+ v_dy_2.v = vec_sub(v_piy.v, v_pjy2.v);
+ v_dz.v = vec_sub(v_piz.v, v_pjz.v);
+ v_dz_2.v = vec_sub(v_piz.v, v_pjz2.v);
v_r2.v = vec_mul(v_dx.v, v_dx.v);
v_r2_2.v = vec_mul(v_dx_2.v, v_dx_2.v);
@@ -500,7 +645,6 @@ __attribute__((always_inline)) INLINE void runner_doself1_density_vec(
/* Form a mask from r2 < hig2 and r2 > 0.*/
mask_t v_doi_mask, v_doi_mask_self_check, v_doi_mask2,
v_doi_mask2_self_check;
- int doi_mask, doi_mask_self_check, doi_mask2, doi_mask2_self_check;
/* Form r2 > 0 mask and r2 < hig2 mask. */
vec_create_mask(v_doi_mask_self_check, vec_cmp_gt(v_r2.v, vec_setzero()));
@@ -511,39 +655,35 @@ __attribute__((always_inline)) INLINE void runner_doself1_density_vec(
vec_cmp_gt(v_r2_2.v, vec_setzero()));
vec_create_mask(v_doi_mask2, vec_cmp_lt(v_r2_2.v, v_hig2.v));
- /* Form integer masks. */
- doi_mask_self_check = vec_form_int_mask(v_doi_mask_self_check);
- doi_mask = vec_form_int_mask(v_doi_mask);
-
- doi_mask2_self_check = vec_form_int_mask(v_doi_mask2_self_check);
- doi_mask2 = vec_form_int_mask(v_doi_mask2);
-
- /* Combine the two masks. */
- doi_mask = doi_mask & doi_mask_self_check;
- doi_mask2 = doi_mask2 & doi_mask2_self_check;
+ /* Combine two masks and form integer masks. */
+ const int doi_mask = vec_is_mask_true(v_doi_mask) &
+ vec_is_mask_true(v_doi_mask_self_check);
+ const int doi_mask2 = vec_is_mask_true(v_doi_mask2) &
+ vec_is_mask_true(v_doi_mask2_self_check);
/* If there are any interactions left pack interaction values into c2
* cache. */
if (doi_mask) {
storeInteractions(doi_mask, pjd, &v_r2, &v_dx, &v_dy, &v_dz, cell_cache,
- &int_cache, &icount, &rhoSum, &rho_dhSum, &wcountSum,
- &wcount_dhSum, &div_vSum, &curlvxSum, &curlvySum,
- &curlvzSum, v_hi_inv, v_vix, v_viy, v_viz);
+ &int_cache, &icount, &v_rhoSum, &v_rho_dhSum,
+ &v_wcountSum, &v_wcount_dhSum, &v_div_vSum,
+ &v_curlvxSum, &v_curlvySum, &v_curlvzSum, v_hi_inv,
+ v_vix, v_viy, v_viz);
}
if (doi_mask2) {
storeInteractions(doi_mask2, pjd + VEC_SIZE, &v_r2_2, &v_dx_2, &v_dy_2,
- &v_dz_2, cell_cache, &int_cache, &icount, &rhoSum,
- &rho_dhSum, &wcountSum, &wcount_dhSum, &div_vSum,
- &curlvxSum, &curlvySum, &curlvzSum, v_hi_inv, v_vix,
- v_viy, v_viz);
+ &v_dz_2, cell_cache, &int_cache, &icount, &v_rhoSum,
+ &v_rho_dhSum, &v_wcountSum, &v_wcount_dhSum,
+ &v_div_vSum, &v_curlvxSum, &v_curlvySum, &v_curlvzSum,
+ v_hi_inv, v_vix, v_viy, v_viz);
}
}
/* Perform padded vector remainder interactions if any are present. */
- calcRemInteractions(&int_cache, icount, &rhoSum, &rho_dhSum, &wcountSum,
- &wcount_dhSum, &div_vSum, &curlvxSum, &curlvySum,
- &curlvzSum, v_hi_inv, v_vix, v_viy, v_viz,
- &icount_align);
+ calcRemInteractions(&int_cache, icount, &v_rhoSum, &v_rho_dhSum,
+ &v_wcountSum, &v_wcount_dhSum, &v_div_vSum,
+ &v_curlvxSum, &v_curlvySum, &v_curlvzSum, v_hi_inv,
+ v_vix, v_viy, v_viz, &icount_align);
/* Initialise masks to true in case remainder interactions have been
* performed. */
@@ -557,21 +697,21 @@ __attribute__((always_inline)) INLINE void runner_doself1_density_vec(
&int_cache.r2q[pjd], &int_cache.dxq[pjd], &int_cache.dyq[pjd],
&int_cache.dzq[pjd], v_hi_inv, v_vix, v_viy, v_viz,
&int_cache.vxq[pjd], &int_cache.vyq[pjd], &int_cache.vzq[pjd],
- &int_cache.mq[pjd], &rhoSum, &rho_dhSum, &wcountSum, &wcount_dhSum,
- &div_vSum, &curlvxSum, &curlvySum, &curlvzSum, int_mask, int_mask2,
- 0);
+ &int_cache.mq[pjd], &v_rhoSum, &v_rho_dhSum, &v_wcountSum,
+ &v_wcount_dhSum, &v_div_vSum, &v_curlvxSum, &v_curlvySum,
+ &v_curlvzSum, int_mask, int_mask2, 0);
}
/* Perform horizontal adds on vector sums and store result in particle pi.
*/
- VEC_HADD(rhoSum, pi->rho);
- VEC_HADD(rho_dhSum, pi->density.rho_dh);
- VEC_HADD(wcountSum, pi->density.wcount);
- VEC_HADD(wcount_dhSum, pi->density.wcount_dh);
- VEC_HADD(div_vSum, pi->density.div_v);
- VEC_HADD(curlvxSum, pi->density.rot_v[0]);
- VEC_HADD(curlvySum, pi->density.rot_v[1]);
- VEC_HADD(curlvzSum, pi->density.rot_v[2]);
+ VEC_HADD(v_rhoSum, pi->rho);
+ VEC_HADD(v_rho_dhSum, pi->density.rho_dh);
+ VEC_HADD(v_wcountSum, pi->density.wcount);
+ VEC_HADD(v_wcount_dhSum, pi->density.wcount_dh);
+ VEC_HADD(v_div_vSum, pi->density.div_v);
+ VEC_HADD(v_curlvxSum, pi->density.rot_v[0]);
+ VEC_HADD(v_curlvySum, pi->density.rot_v[1]);
+ VEC_HADD(v_curlvzSum, pi->density.rot_v[2]);
/* Reset interaction count. */
icount = 0;
@@ -602,9 +742,6 @@ __attribute__((always_inline)) INLINE void runner_doself2_force_vec(
struct part *restrict parts = c->parts;
const int count = c->count;
- vector v_hi, v_vix, v_viy, v_viz, v_hig2, v_r2;
- vector v_rhoi, v_grad_hi, v_pOrhoi2, v_balsara_i, v_ci;
-
TIMER_TIC;
if (!cell_is_active(c, e)) return;
@@ -640,43 +777,36 @@ __attribute__((always_inline)) INLINE void runner_doself2_force_vec(
/* Is the ith particle active? */
if (!part_is_active_no_debug(pi, max_active_bin)) continue;
- vector pix, piy, piz;
-
const float hi = cell_cache->h[pid];
/* Fill particle pi vectors. */
- pix.v = vec_set1(cell_cache->x[pid]);
- piy.v = vec_set1(cell_cache->y[pid]);
- piz.v = vec_set1(cell_cache->z[pid]);
- v_hi.v = vec_set1(hi);
- v_vix.v = vec_set1(cell_cache->vx[pid]);
- v_viy.v = vec_set1(cell_cache->vy[pid]);
- v_viz.v = vec_set1(cell_cache->vz[pid]);
-
- v_rhoi.v = vec_set1(cell_cache->rho[pid]);
- v_grad_hi.v = vec_set1(cell_cache->grad_h[pid]);
- v_pOrhoi2.v = vec_set1(cell_cache->pOrho2[pid]);
- v_balsara_i.v = vec_set1(cell_cache->balsara[pid]);
- v_ci.v = vec_set1(cell_cache->soundspeed[pid]);
+ const vector v_pix = vector_set1(cell_cache->x[pid]);
+ const vector v_piy = vector_set1(cell_cache->y[pid]);
+ const vector v_piz = vector_set1(cell_cache->z[pid]);
+ const vector v_hi = vector_set1(hi);
+ const vector v_vix = vector_set1(cell_cache->vx[pid]);
+ const vector v_viy = vector_set1(cell_cache->vy[pid]);
+ const vector v_viz = vector_set1(cell_cache->vz[pid]);
+
+ const vector v_rhoi = vector_set1(cell_cache->rho[pid]);
+ const vector v_grad_hi = vector_set1(cell_cache->grad_h[pid]);
+ const vector v_pOrhoi2 = vector_set1(cell_cache->pOrho2[pid]);
+ const vector v_balsara_i = vector_set1(cell_cache->balsara[pid]);
+ const vector v_ci = vector_set1(cell_cache->soundspeed[pid]);
const float hig2 = hi * hi * kernel_gamma2;
- v_hig2.v = vec_set1(hig2);
-
- /* Reset cumulative sums of update vectors. */
- vector a_hydro_xSum, a_hydro_ySum, a_hydro_zSum, h_dtSum, v_sigSum,
- entropy_dtSum;
+ const vector v_hig2 = vector_set1(hig2);
/* Get the inverse of hi. */
- vector v_hi_inv;
-
- v_hi_inv = vec_reciprocal(v_hi);
+ vector v_hi_inv = vec_reciprocal(v_hi);
- a_hydro_xSum.v = vec_setzero();
- a_hydro_ySum.v = vec_setzero();
- a_hydro_zSum.v = vec_setzero();
- h_dtSum.v = vec_setzero();
- v_sigSum.v = vec_set1(pi->force.v_sig);
- entropy_dtSum.v = vec_setzero();
+ /* Reset cumulative sums of update vectors. */
+ vector v_a_hydro_xSum = vector_setzero();
+ vector v_a_hydro_ySum = vector_setzero();
+ vector v_a_hydro_zSum = vector_setzero();
+ vector v_h_dtSum = vector_setzero();
+ vector v_sigSum = vector_set1(pi->force.v_sig);
+ vector v_entropy_dtSum = vector_setzero();
/* Pad cache if there is a serial remainder. */
count_align = count;
@@ -689,9 +819,9 @@ __attribute__((always_inline)) INLINE void runner_doself2_force_vec(
/* Set positions to the same as particle pi so when the r2 > 0 mask is
* applied these extra contributions are masked out.*/
for (int i = count; i < count_align; i++) {
- cell_cache->x[i] = pix.f[0];
- cell_cache->y[i] = piy.f[0];
- cell_cache->z[i] = piz.f[0];
+ cell_cache->x[i] = v_pix.f[0];
+ cell_cache->y[i] = v_piy.f[0];
+ cell_cache->z[i] = v_piz.f[0];
cell_cache->h[i] = 1.f;
cell_cache->rho[i] = 1.f;
cell_cache->grad_h[i] = 1.f;
@@ -701,25 +831,23 @@ __attribute__((always_inline)) INLINE void runner_doself2_force_vec(
}
}
- vector pjx, pjy, pjz, hj, hjg2;
-
/* Find all of particle pi's interacions and store needed values in the
* secondary cache.*/
for (int pjd = 0; pjd < count_align; pjd += (num_vec_proc * VEC_SIZE)) {
/* Load 1 set of vectors from the particle cache. */
- pjx.v = vec_load(&cell_cache->x[pjd]);
- pjy.v = vec_load(&cell_cache->y[pjd]);
- pjz.v = vec_load(&cell_cache->z[pjd]);
- hj.v = vec_load(&cell_cache->h[pjd]);
+ vector hjg2;
+ const vector v_pjx = vector_load(&cell_cache->x[pjd]);
+ const vector v_pjy = vector_load(&cell_cache->y[pjd]);
+ const vector v_pjz = vector_load(&cell_cache->z[pjd]);
+ const vector hj = vector_load(&cell_cache->h[pjd]);
hjg2.v = vec_mul(vec_mul(hj.v, hj.v), kernel_gamma2_vec.v);
/* Compute the pairwise distance. */
- vector v_dx, v_dy, v_dz;
-
- v_dx.v = vec_sub(pix.v, pjx.v);
- v_dy.v = vec_sub(piy.v, pjy.v);
- v_dz.v = vec_sub(piz.v, pjz.v);
+ vector v_dx, v_dy, v_dz, v_r2;
+ v_dx.v = vec_sub(v_pix.v, v_pjx.v);
+ v_dy.v = vec_sub(v_piy.v, v_pjy.v);
+ v_dz.v = vec_sub(v_piz.v, v_pjz.v);
v_r2.v = vec_mul(v_dx.v, v_dx.v);
v_r2.v = vec_fma(v_dy.v, v_dy.v, v_r2.v);
@@ -727,7 +855,6 @@ __attribute__((always_inline)) INLINE void runner_doself2_force_vec(
/* Form r2 > 0 mask, r2 < hig2 mask and r2 < hjg2 mask. */
mask_t v_doi_mask, v_doi_mask_self_check;
- int doi_mask;
/* Form r2 > 0 mask.*/
vec_create_mask(v_doi_mask_self_check, vec_cmp_gt(v_r2.v, vec_setzero()));
@@ -737,18 +864,15 @@ __attribute__((always_inline)) INLINE void runner_doself2_force_vec(
v_h2.v = vec_fmax(v_hig2.v, hjg2.v);
vec_create_mask(v_doi_mask, vec_cmp_lt(v_r2.v, v_h2.v));
- /* Combine all 3 masks and form integer mask. */
+ /* Combine all 3 masks. */
vec_combine_masks(v_doi_mask, v_doi_mask_self_check);
- doi_mask = vec_form_int_mask(v_doi_mask);
/* If there are any interactions perform them. */
- if (doi_mask) {
- vector v_hj_inv;
- v_hj_inv = vec_reciprocal(hj);
+ if (vec_is_mask_true(v_doi_mask)) {
+ vector v_hj_inv = vec_reciprocal(hj);
/* To stop floating point exceptions for when particle separations are
- * 0.
- */
+ * 0. */
v_r2.v = vec_add(v_r2.v, vec_set1(FLT_MIN));
runner_iact_nonsym_1_vec_force(
@@ -757,19 +881,19 @@ __attribute__((always_inline)) INLINE void runner_doself2_force_vec(
&cell_cache->vy[pjd], &cell_cache->vz[pjd], &cell_cache->rho[pjd],
&cell_cache->grad_h[pjd], &cell_cache->pOrho2[pjd],
&cell_cache->balsara[pjd], &cell_cache->soundspeed[pjd],
- &cell_cache->m[pjd], v_hi_inv, v_hj_inv, &a_hydro_xSum,
- &a_hydro_ySum, &a_hydro_zSum, &h_dtSum, &v_sigSum, &entropy_dtSum,
- v_doi_mask);
+ &cell_cache->m[pjd], v_hi_inv, v_hj_inv, &v_a_hydro_xSum,
+ &v_a_hydro_ySum, &v_a_hydro_zSum, &v_h_dtSum, &v_sigSum,
+ &v_entropy_dtSum, v_doi_mask);
}
} /* Loop over all other particles. */
- VEC_HADD(a_hydro_xSum, pi->a_hydro[0]);
- VEC_HADD(a_hydro_ySum, pi->a_hydro[1]);
- VEC_HADD(a_hydro_zSum, pi->a_hydro[2]);
- VEC_HADD(h_dtSum, pi->force.h_dt);
+ VEC_HADD(v_a_hydro_xSum, pi->a_hydro[0]);
+ VEC_HADD(v_a_hydro_ySum, pi->a_hydro[1]);
+ VEC_HADD(v_a_hydro_zSum, pi->a_hydro[2]);
+ VEC_HADD(v_h_dtSum, pi->force.h_dt);
VEC_HMAX(v_sigSum, pi->force.v_sig);
- VEC_HADD(entropy_dtSum, pi->entropy_dt);
+ VEC_HADD(v_entropy_dtSum, pi->entropy_dt);
} /* loop over all particles. */
@@ -795,8 +919,6 @@ void runner_dopair1_density_vec(struct runner *r, struct cell *ci,
const struct engine *restrict e = r->e;
const timebin_t max_active_bin = e->max_active_bin;
- vector v_hi, v_vix, v_viy, v_viz, v_hig2;
-
TIMER_TIC;
/* Get the cutoff shift. */
@@ -807,39 +929,6 @@ void runner_dopair1_density_vec(struct runner *r, struct cell *ci,
const struct entry *restrict sort_i = ci->sort[sid];
const struct entry *restrict sort_j = cj->sort[sid];
-#ifdef SWIFT_DEBUG_CHECKS
- /* Check that the dx_max_sort values in the cell are indeed an upper
- bound on particle movement. */
- for (int pid = 0; pid < ci->count; pid++) {
- const struct part *p = &ci->parts[sort_i[pid].i];
- const float d = p->x[0] * runner_shift[sid][0] +
- p->x[1] * runner_shift[sid][1] +
- p->x[2] * runner_shift[sid][2];
- if (fabsf(d - sort_i[pid].d) - ci->dx_max_sort >
- 1.0e-4 * max(fabsf(d), ci->dx_max_sort_old))
- error(
- "particle shift diff exceeds dx_max_sort in cell ci. ci->nodeID=%d "
- "cj->nodeID=%d d=%e sort_i[pid].d=%e ci->dx_max_sort=%e "
- "ci->dx_max_sort_old=%e",
- ci->nodeID, cj->nodeID, d, sort_i[pid].d, ci->dx_max_sort,
- ci->dx_max_sort_old);
- }
- for (int pjd = 0; pjd < cj->count; pjd++) {
- const struct part *p = &cj->parts[sort_j[pjd].i];
- const float d = p->x[0] * runner_shift[sid][0] +
- p->x[1] * runner_shift[sid][1] +
- p->x[2] * runner_shift[sid][2];
- if (fabsf(d - sort_j[pjd].d) - cj->dx_max_sort >
- 1.0e-4 * max(fabsf(d), cj->dx_max_sort_old))
- error(
- "particle shift diff exceeds dx_max_sort in cell cj. cj->nodeID=%d "
- "ci->nodeID=%d d=%e sort_j[pjd].d=%e cj->dx_max_sort=%e "
- "cj->dx_max_sort_old=%e",
- cj->nodeID, ci->nodeID, d, sort_j[pjd].d, cj->dx_max_sort,
- cj->dx_max_sort_old);
- }
-#endif /* SWIFT_DEBUG_CHECKS */
-
/* Get some other useful values. */
const int count_i = ci->count;
const int count_j = cj->count;
@@ -853,7 +942,7 @@ void runner_dopair1_density_vec(struct runner *r, struct cell *ci,
const int active_ci = cell_is_active(ci, e);
const int active_cj = cell_is_active(cj, e);
- /* Check if any particles are active and return if there are not. */
+ /* Count number of particles that are in range and active*/
int numActive = 0;
if (active_ci) {
@@ -878,6 +967,7 @@ void runner_dopair1_density_vec(struct runner *r, struct cell *ci,
}
}
+ /* Return if there are no active particles within range */
if (numActive == 0) return;
/* Get both particle caches from the runner and re-allocate
@@ -900,8 +990,7 @@ void runner_dopair1_density_vec(struct runner *r, struct cell *ci,
max_index_j = r->cj_cache.max_index;
/* Find particles maximum index into cj, max_index_i[] and ci, max_index_j[].
- */
- /* Also find the first pi that interacts with any particle in cj and the last
+ * Also find the first pi that interacts with any particle in cj and the last
* pj that interacts with any particle in ci. */
populate_max_index_no_cache(ci, cj, sort_i, sort_j, dx_max, rshift, hi_max,
hj_max, di_max, dj_min, max_index_i, max_index_j,
@@ -916,15 +1005,12 @@ void runner_dopair1_density_vec(struct runner *r, struct cell *ci,
last_pj = max(last_pj, max_index_i[count_i - 1]);
first_pi = min(first_pi, max_index_j[0]);
- /* Read the needed particles into the two caches. */
- int first_pi_align = first_pi;
- int last_pj_align = last_pj;
+ /* Read the required particles into the two caches. */
cache_read_two_partial_cells_sorted(ci, cj, ci_cache, cj_cache, sort_i,
- sort_j, shift, &first_pi_align,
- &last_pj_align, 1);
+ sort_j, shift, &first_pi, &last_pj);
/* Get the number of particles read into the ci cache. */
- int ci_cache_count = count_i - first_pi_align;
+ const int ci_cache_count = count_i - first_pi;
if (active_ci) {
@@ -936,7 +1022,7 @@ void runner_dopair1_density_vec(struct runner *r, struct cell *ci,
if (!part_is_active_no_debug(pi, max_active_bin)) continue;
/* Set the cache index. */
- int ci_cache_idx = pid - first_pi_align;
+ const int ci_cache_idx = pid - first_pi;
/* Skip this particle if no particle in cj is within range of it. */
const float hi = ci_cache->h[ci_cache_idx];
@@ -945,113 +1031,101 @@ void runner_dopair1_density_vec(struct runner *r, struct cell *ci,
if (di_test < dj_min) continue;
/* Determine the exit iteration of the interaction loop. */
- int exit_iteration = max_index_i[pid];
-
- const float hig2 = hi * hi * kernel_gamma2;
-
- vector pix, piy, piz;
+ const int exit_iteration = max_index_i[pid];
/* Fill particle pi vectors. */
- pix.v = vec_set1(ci_cache->x[ci_cache_idx]);
- piy.v = vec_set1(ci_cache->y[ci_cache_idx]);
- piz.v = vec_set1(ci_cache->z[ci_cache_idx]);
- v_hi.v = vec_set1(hi);
- v_vix.v = vec_set1(ci_cache->vx[ci_cache_idx]);
- v_viy.v = vec_set1(ci_cache->vy[ci_cache_idx]);
- v_viz.v = vec_set1(ci_cache->vz[ci_cache_idx]);
-
- v_hig2.v = vec_set1(hig2);
+ const vector v_pix = vector_set1(ci_cache->x[ci_cache_idx]);
+ const vector v_piy = vector_set1(ci_cache->y[ci_cache_idx]);
+ const vector v_piz = vector_set1(ci_cache->z[ci_cache_idx]);
+ const vector v_hi = vector_set1(hi);
+ const vector v_vix = vector_set1(ci_cache->vx[ci_cache_idx]);
+ const vector v_viy = vector_set1(ci_cache->vy[ci_cache_idx]);
+ const vector v_viz = vector_set1(ci_cache->vz[ci_cache_idx]);
- /* Reset cumulative sums of update vectors. */
- vector rhoSum, rho_dhSum, wcountSum, wcount_dhSum, div_vSum, curlvxSum,
- curlvySum, curlvzSum;
+ const float hig2 = hi * hi * kernel_gamma2;
+ const vector v_hig2 = vector_set1(hig2);
/* Get the inverse of hi. */
- vector v_hi_inv;
-
- v_hi_inv = vec_reciprocal(v_hi);
+ vector v_hi_inv = vec_reciprocal(v_hi);
- rhoSum.v = vec_setzero();
- rho_dhSum.v = vec_setzero();
- wcountSum.v = vec_setzero();
- wcount_dhSum.v = vec_setzero();
- div_vSum.v = vec_setzero();
- curlvxSum.v = vec_setzero();
- curlvySum.v = vec_setzero();
- curlvzSum.v = vec_setzero();
+ /* Reset cumulative sums of update vectors. */
+ vector v_rhoSum = vector_setzero();
+ vector v_rho_dhSum = vector_setzero();
+ vector v_wcountSum = vector_setzero();
+ vector v_wcount_dhSum = vector_setzero();
+ vector v_div_vSum = vector_setzero();
+ vector v_curlvxSum = vector_setzero();
+ vector v_curlvySum = vector_setzero();
+ vector v_curlvzSum = vector_setzero();
/* Pad the exit iteration if there is a serial remainder. */
int exit_iteration_align = exit_iteration;
- int rem = exit_iteration % VEC_SIZE;
+ const int rem = exit_iteration % VEC_SIZE;
if (rem != 0) {
- int pad = VEC_SIZE - rem;
+ const int pad = VEC_SIZE - rem;
- if (exit_iteration_align + pad <= last_pj_align + 1)
+ if (exit_iteration_align + pad <= last_pj + 1)
exit_iteration_align += pad;
}
- vector pjx, pjy, pjz;
-
- /* Loop over the parts in cj. */
- for (int pjd = 0; pjd < exit_iteration_align; pjd += VEC_SIZE) {
+ /* Loop over the parts in cj. Making sure to perform an iteration of the
+ * loop even if exit_iteration_align is zero and there is only one
+ * particle to interact with.*/
+ for (int pjd = 0; pjd <= exit_iteration_align; pjd += VEC_SIZE) {
/* Get the cache index to the jth particle. */
- int cj_cache_idx = pjd;
+ const int cj_cache_idx = pjd;
vector v_dx, v_dy, v_dz, v_r2;
#ifdef SWIFT_DEBUG_CHECKS
if (cj_cache_idx % VEC_SIZE != 0 || cj_cache_idx < 0 ||
- cj_cache_idx + (VEC_SIZE - 1) > (last_pj_align + 1 + VEC_SIZE)) {
- error("Unaligned read!!! cj_cache_idx=%d, last_pj_align=%d",
- cj_cache_idx, last_pj_align);
+ cj_cache_idx + (VEC_SIZE - 1) > (last_pj + 1 + VEC_SIZE)) {
+ error("Unaligned read!!! cj_cache_idx=%d, last_pj=%d", cj_cache_idx,
+ last_pj);
}
#endif
/* Load 2 sets of vectors from the particle cache. */
- pjx.v = vec_load(&cj_cache->x[cj_cache_idx]);
- pjy.v = vec_load(&cj_cache->y[cj_cache_idx]);
- pjz.v = vec_load(&cj_cache->z[cj_cache_idx]);
+ const vector v_pjx = vector_load(&cj_cache->x[cj_cache_idx]);
+ const vector v_pjy = vector_load(&cj_cache->y[cj_cache_idx]);
+ const vector v_pjz = vector_load(&cj_cache->z[cj_cache_idx]);
/* Compute the pairwise distance. */
- v_dx.v = vec_sub(pix.v, pjx.v);
- v_dy.v = vec_sub(piy.v, pjy.v);
- v_dz.v = vec_sub(piz.v, pjz.v);
+ v_dx.v = vec_sub(v_pix.v, v_pjx.v);
+ v_dy.v = vec_sub(v_piy.v, v_pjy.v);
+ v_dz.v = vec_sub(v_piz.v, v_pjz.v);
v_r2.v = vec_mul(v_dx.v, v_dx.v);
v_r2.v = vec_fma(v_dy.v, v_dy.v, v_r2.v);
v_r2.v = vec_fma(v_dz.v, v_dz.v, v_r2.v);
mask_t v_doi_mask;
- int doi_mask;
/* Form r2 < hig2 mask. */
vec_create_mask(v_doi_mask, vec_cmp_lt(v_r2.v, v_hig2.v));
- /* Form integer mask. */
- doi_mask = vec_form_int_mask(v_doi_mask);
-
/* If there are any interactions perform them. */
- if (doi_mask)
+ if (vec_is_mask_true(v_doi_mask))
runner_iact_nonsym_1_vec_density(
&v_r2, &v_dx, &v_dy, &v_dz, v_hi_inv, v_vix, v_viy, v_viz,
&cj_cache->vx[cj_cache_idx], &cj_cache->vy[cj_cache_idx],
- &cj_cache->vz[cj_cache_idx], &cj_cache->m[cj_cache_idx], &rhoSum,
- &rho_dhSum, &wcountSum, &wcount_dhSum, &div_vSum, &curlvxSum,
- &curlvySum, &curlvzSum, v_doi_mask);
+ &cj_cache->vz[cj_cache_idx], &cj_cache->m[cj_cache_idx],
+ &v_rhoSum, &v_rho_dhSum, &v_wcountSum, &v_wcount_dhSum,
+ &v_div_vSum, &v_curlvxSum, &v_curlvySum, &v_curlvzSum,
+ v_doi_mask);
} /* loop over the parts in cj. */
- /* Perform horizontal adds on vector sums and store result in particle pi.
- */
- VEC_HADD(rhoSum, pi->rho);
- VEC_HADD(rho_dhSum, pi->density.rho_dh);
- VEC_HADD(wcountSum, pi->density.wcount);
- VEC_HADD(wcount_dhSum, pi->density.wcount_dh);
- VEC_HADD(div_vSum, pi->density.div_v);
- VEC_HADD(curlvxSum, pi->density.rot_v[0]);
- VEC_HADD(curlvySum, pi->density.rot_v[1]);
- VEC_HADD(curlvzSum, pi->density.rot_v[2]);
+ /* Perform horizontal adds on vector sums and store result in pi. */
+ VEC_HADD(v_rhoSum, pi->rho);
+ VEC_HADD(v_rho_dhSum, pi->density.rho_dh);
+ VEC_HADD(v_wcountSum, pi->density.wcount);
+ VEC_HADD(v_wcount_dhSum, pi->density.wcount_dh);
+ VEC_HADD(v_div_vSum, pi->density.div_v);
+ VEC_HADD(v_curlvxSum, pi->density.rot_v[0]);
+ VEC_HADD(v_curlvySum, pi->density.rot_v[1]);
+ VEC_HADD(v_curlvzSum, pi->density.rot_v[2]);
} /* loop over the parts in ci. */
}
@@ -1066,7 +1140,7 @@ void runner_dopair1_density_vec(struct runner *r, struct cell *ci,
if (!part_is_active_no_debug(pj, max_active_bin)) continue;
/* Set the cache index. */
- int cj_cache_idx = pjd;
+ const int cj_cache_idx = pjd;
/* Skip this particle if no particle in ci is within range of it. */
const float hj = cj_cache->h[cj_cache_idx];
@@ -1074,49 +1148,38 @@ void runner_dopair1_density_vec(struct runner *r, struct cell *ci,
if (dj_test > di_max) continue;
/* Determine the exit iteration of the interaction loop. */
- int exit_iteration = max_index_j[pjd];
-
- const float hjg2 = hj * hj * kernel_gamma2;
-
- vector pjx, pjy, pjz;
- vector v_hj, v_vjx, v_vjy, v_vjz, v_hjg2;
+ const int exit_iteration = max_index_j[pjd];
/* Fill particle pi vectors. */
- pjx.v = vec_set1(cj_cache->x[cj_cache_idx]);
- pjy.v = vec_set1(cj_cache->y[cj_cache_idx]);
- pjz.v = vec_set1(cj_cache->z[cj_cache_idx]);
- v_hj.v = vec_set1(hj);
- v_vjx.v = vec_set1(cj_cache->vx[cj_cache_idx]);
- v_vjy.v = vec_set1(cj_cache->vy[cj_cache_idx]);
- v_vjz.v = vec_set1(cj_cache->vz[cj_cache_idx]);
+ const vector v_pjx = vector_set1(cj_cache->x[cj_cache_idx]);
+ const vector v_pjy = vector_set1(cj_cache->y[cj_cache_idx]);
+ const vector v_pjz = vector_set1(cj_cache->z[cj_cache_idx]);
+ const vector v_hj = vector_set1(hj);
+ const vector v_vjx = vector_set1(cj_cache->vx[cj_cache_idx]);
+ const vector v_vjy = vector_set1(cj_cache->vy[cj_cache_idx]);
+ const vector v_vjz = vector_set1(cj_cache->vz[cj_cache_idx]);
- v_hjg2.v = vec_set1(hjg2);
-
- /* Reset cumulative sums of update vectors. */
- vector rhoSum, rho_dhSum, wcountSum, wcount_dhSum, div_vSum, curlvxSum,
- curlvySum, curlvzSum;
+ const float hjg2 = hj * hj * kernel_gamma2;
+ const vector v_hjg2 = vector_set1(hjg2);
/* Get the inverse of hj. */
- vector v_hj_inv;
+ vector v_hj_inv = vec_reciprocal(v_hj);
- v_hj_inv = vec_reciprocal(v_hj);
-
- rhoSum.v = vec_setzero();
- rho_dhSum.v = vec_setzero();
- wcountSum.v = vec_setzero();
- wcount_dhSum.v = vec_setzero();
- div_vSum.v = vec_setzero();
- curlvxSum.v = vec_setzero();
- curlvySum.v = vec_setzero();
- curlvzSum.v = vec_setzero();
-
- vector pix, piy, piz;
+ /* Reset cumulative sums of update vectors. */
+ vector v_rhoSum = vector_setzero();
+ vector v_rho_dhSum = vector_setzero();
+ vector v_wcountSum = vector_setzero();
+ vector v_wcount_dhSum = vector_setzero();
+ vector v_div_vSum = vector_setzero();
+ vector v_curlvxSum = vector_setzero();
+ vector v_curlvySum = vector_setzero();
+ vector v_curlvzSum = vector_setzero();
/* Convert exit iteration to cache indices. */
- int exit_iteration_align = exit_iteration - first_pi_align;
+ int exit_iteration_align = exit_iteration - first_pi;
/* Pad the exit iteration align so cache reads are aligned. */
- int rem = exit_iteration_align % VEC_SIZE;
+ const int rem = exit_iteration_align % VEC_SIZE;
if (exit_iteration_align < VEC_SIZE) {
exit_iteration_align = 0;
} else
@@ -1128,61 +1191,56 @@ void runner_dopair1_density_vec(struct runner *r, struct cell *ci,
#ifdef SWIFT_DEBUG_CHECKS
if (ci_cache_idx % VEC_SIZE != 0 || ci_cache_idx < 0 ||
- ci_cache_idx + (VEC_SIZE - 1) >
- (count_i - first_pi_align + VEC_SIZE)) {
+ ci_cache_idx + (VEC_SIZE - 1) > (count_i - first_pi + VEC_SIZE)) {
error(
- "Unaligned read!!! ci_cache_idx=%d, first_pi_align=%d, "
+ "Unaligned read!!! ci_cache_idx=%d, first_pi=%d, "
"count_i=%d",
- ci_cache_idx, first_pi_align, count_i);
+ ci_cache_idx, first_pi, count_i);
}
#endif
vector v_dx, v_dy, v_dz, v_r2;
/* Load 2 sets of vectors from the particle cache. */
- pix.v = vec_load(&ci_cache->x[ci_cache_idx]);
- piy.v = vec_load(&ci_cache->y[ci_cache_idx]);
- piz.v = vec_load(&ci_cache->z[ci_cache_idx]);
+ const vector v_pix = vector_load(&ci_cache->x[ci_cache_idx]);
+ const vector v_piy = vector_load(&ci_cache->y[ci_cache_idx]);
+ const vector v_piz = vector_load(&ci_cache->z[ci_cache_idx]);
/* Compute the pairwise distance. */
- v_dx.v = vec_sub(pjx.v, pix.v);
- v_dy.v = vec_sub(pjy.v, piy.v);
- v_dz.v = vec_sub(pjz.v, piz.v);
+ v_dx.v = vec_sub(v_pjx.v, v_pix.v);
+ v_dy.v = vec_sub(v_pjy.v, v_piy.v);
+ v_dz.v = vec_sub(v_pjz.v, v_piz.v);
v_r2.v = vec_mul(v_dx.v, v_dx.v);
v_r2.v = vec_fma(v_dy.v, v_dy.v, v_r2.v);
v_r2.v = vec_fma(v_dz.v, v_dz.v, v_r2.v);
mask_t v_doj_mask;
- int doj_mask;
/* Form r2 < hig2 mask. */
vec_create_mask(v_doj_mask, vec_cmp_lt(v_r2.v, v_hjg2.v));
- /* Form integer mask. */
- doj_mask = vec_form_int_mask(v_doj_mask);
-
/* If there are any interactions perform them. */
- if (doj_mask)
+ if (vec_is_mask_true(v_doj_mask))
runner_iact_nonsym_1_vec_density(
&v_r2, &v_dx, &v_dy, &v_dz, v_hj_inv, v_vjx, v_vjy, v_vjz,
&ci_cache->vx[ci_cache_idx], &ci_cache->vy[ci_cache_idx],
- &ci_cache->vz[ci_cache_idx], &ci_cache->m[ci_cache_idx], &rhoSum,
- &rho_dhSum, &wcountSum, &wcount_dhSum, &div_vSum, &curlvxSum,
- &curlvySum, &curlvzSum, v_doj_mask);
+ &ci_cache->vz[ci_cache_idx], &ci_cache->m[ci_cache_idx],
+ &v_rhoSum, &v_rho_dhSum, &v_wcountSum, &v_wcount_dhSum,
+ &v_div_vSum, &v_curlvxSum, &v_curlvySum, &v_curlvzSum,
+ v_doj_mask);
} /* loop over the parts in ci. */
- /* Perform horizontal adds on vector sums and store result in particle pj.
- */
- VEC_HADD(rhoSum, pj->rho);
- VEC_HADD(rho_dhSum, pj->density.rho_dh);
- VEC_HADD(wcountSum, pj->density.wcount);
- VEC_HADD(wcount_dhSum, pj->density.wcount_dh);
- VEC_HADD(div_vSum, pj->density.div_v);
- VEC_HADD(curlvxSum, pj->density.rot_v[0]);
- VEC_HADD(curlvySum, pj->density.rot_v[1]);
- VEC_HADD(curlvzSum, pj->density.rot_v[2]);
+ /* Perform horizontal adds on vector sums and store result in pj. */
+ VEC_HADD(v_rhoSum, pj->rho);
+ VEC_HADD(v_rho_dhSum, pj->density.rho_dh);
+ VEC_HADD(v_wcountSum, pj->density.wcount);
+ VEC_HADD(v_wcount_dhSum, pj->density.wcount_dh);
+ VEC_HADD(v_div_vSum, pj->density.div_v);
+ VEC_HADD(v_curlvxSum, pj->density.rot_v[0]);
+ VEC_HADD(v_curlvySum, pj->density.rot_v[1]);
+ VEC_HADD(v_curlvzSum, pj->density.rot_v[2]);
} /* loop over the parts in cj. */
}
@@ -1191,3 +1249,381 @@ void runner_dopair1_density_vec(struct runner *r, struct cell *ci,
#endif /* WITH_VECTORIZATION */
}
+
+/**
+ * @brief Compute the force interactions between a cell pair (non-symmetric)
+ * using vector intrinsics.
+ *
+ * @param r The #runner.
+ * @param ci The first #cell.
+ * @param cj The second #cell.
+ * @param sid The direction of the pair
+ * @param shift The shift vector to apply to the particles in ci.
+ */
+void runner_dopair2_force_vec(struct runner *r, struct cell *ci,
+ struct cell *cj, const int sid,
+ const double *shift) {
+
+#ifdef WITH_VECTORIZATION
+ const struct engine *restrict e = r->e;
+ const timebin_t max_active_bin = e->max_active_bin;
+
+ TIMER_TIC;
+
+ /* Get the cutoff shift. */
+ double rshift = 0.0;
+ for (int k = 0; k < 3; k++) rshift += shift[k] * runner_shift[sid][k];
+
+ /* Pick-out the sorted lists. */
+ const struct entry *restrict sort_i = ci->sort[sid];
+ const struct entry *restrict sort_j = cj->sort[sid];
+
+ /* Get some other useful values. */
+ const int count_i = ci->count;
+ const int count_j = cj->count;
+ const double hi_max = ci->h_max * kernel_gamma - rshift;
+ const double hj_max = cj->h_max * kernel_gamma;
+ const double hi_max_raw = ci->h_max;
+ const double hj_max_raw = cj->h_max;
+ struct part *restrict parts_i = ci->parts;
+ struct part *restrict parts_j = cj->parts;
+ const double di_max = sort_i[count_i - 1].d - rshift;
+ const double dj_min = sort_j[0].d;
+ const float dx_max = (ci->dx_max_sort + cj->dx_max_sort);
+ const int active_ci = cell_is_active(ci, e);
+ const int active_cj = cell_is_active(cj, e);
+
+ /* Check if any particles are active and in range */
+ int numActive = 0;
+
+ /* Use the largest smoothing length to make sure that no interactions are
+ * missed. */
+ const double h_max = max(hi_max, hj_max);
+
+ if (active_ci) {
+ for (int pid = count_i - 1;
+ pid >= 0 && sort_i[pid].d + h_max + dx_max > dj_min; pid--) {
+ struct part *restrict pi = &parts_i[sort_i[pid].i];
+ if (part_is_active(pi, e)) {
+ numActive++;
+ break;
+ }
+ }
+ }
+
+ if (!numActive && active_cj) {
+ for (int pjd = 0; pjd < count_j && sort_j[pjd].d - h_max - dx_max < di_max;
+ pjd++) {
+ struct part *restrict pj = &parts_j[sort_j[pjd].i];
+ if (part_is_active_no_debug(pj, max_active_bin)) {
+ numActive++;
+ break;
+ }
+ }
+ }
+
+ /* Return if no active particle in range */
+ if (numActive == 0) return;
+
+ /* Get both particle caches from the runner and re-allocate
+ * them if they are not big enough for the cells. */
+ struct cache *restrict ci_cache = &r->ci_cache;
+ struct cache *restrict cj_cache = &r->cj_cache;
+
+ if (ci_cache->count < count_i) {
+ cache_init(ci_cache, count_i);
+ }
+ if (cj_cache->count < count_j) {
+ cache_init(cj_cache, count_j);
+ }
+
+ int first_pi, last_pj;
+ int *max_index_i SWIFT_CACHE_ALIGN;
+ int *max_index_j SWIFT_CACHE_ALIGN;
+
+ max_index_i = r->ci_cache.max_index;
+ max_index_j = r->cj_cache.max_index;
+
+ /* Find particles maximum distance into cj, max_di[] and ci, max_dj[]. */
+ /* Also find the first pi that interacts with any particle in cj and the last
+ * pj that interacts with any particle in ci. */
+ populate_max_index_no_cache_force(ci, cj, sort_i, sort_j, dx_max, rshift,
+ hi_max_raw, hj_max_raw, hi_max, hj_max,
+ di_max, dj_min, max_index_i, max_index_j,
+ &first_pi, &last_pj, max_active_bin);
+
+ /* Limits of the outer loops. */
+ const int first_pi_loop = first_pi;
+ const int last_pj_loop = last_pj;
+
+ /* Take the max/min of both values calculated to work out how many particles
+ * to read into the cache. */
+ last_pj = max(last_pj, max_index_i[count_i - 1]);
+ first_pi = min(first_pi, max_index_j[0]);
+
+ /* Read the required particles into the two caches. */
+ cache_read_two_partial_cells_sorted_force(ci, cj, ci_cache, cj_cache, sort_i,
+ sort_j, shift, &first_pi, &last_pj);
+
+ /* Get the number of particles read into the ci cache. */
+ const int ci_cache_count = count_i - first_pi;
+
+ if (active_ci) {
+
+ /* Loop over the parts in ci until nothing is within range in cj. */
+ for (int pid = count_i - 1; pid >= first_pi_loop; pid--) {
+
+ /* Get a hold of the ith part in ci. */
+ struct part *restrict pi = &parts_i[sort_i[pid].i];
+ if (!part_is_active(pi, e)) continue;
+
+ /* Set the cache index. */
+ const int ci_cache_idx = pid - first_pi;
+
+ /* Skip this particle if no particle in cj is within range of it. */
+ const float hi = ci_cache->h[ci_cache_idx];
+ const double di_test =
+ sort_i[pid].d + max(hi, hj_max_raw) * kernel_gamma + dx_max - rshift;
+ if (di_test < dj_min) continue;
+
+ /* Determine the exit iteration of the interaction loop. */
+ const int exit_iteration = max_index_i[pid];
+
+ /* Fill particle pi vectors. */
+ const vector v_pix = vector_set1(ci_cache->x[ci_cache_idx]);
+ const vector v_piy = vector_set1(ci_cache->y[ci_cache_idx]);
+ const vector v_piz = vector_set1(ci_cache->z[ci_cache_idx]);
+ const vector v_hi = vector_set1(hi);
+ const vector v_vix = vector_set1(ci_cache->vx[ci_cache_idx]);
+ const vector v_viy = vector_set1(ci_cache->vy[ci_cache_idx]);
+ const vector v_viz = vector_set1(ci_cache->vz[ci_cache_idx]);
+ const vector v_rhoi = vector_set1(ci_cache->rho[ci_cache_idx]);
+ const vector v_grad_hi = vector_set1(ci_cache->grad_h[ci_cache_idx]);
+ const vector v_pOrhoi2 = vector_set1(ci_cache->pOrho2[ci_cache_idx]);
+ const vector v_balsara_i = vector_set1(ci_cache->balsara[ci_cache_idx]);
+ const vector v_ci = vector_set1(ci_cache->soundspeed[ci_cache_idx]);
+
+ const float hig2 = hi * hi * kernel_gamma2;
+ const vector v_hig2 = vector_set1(hig2);
+
+ /* Get the inverse of hi. */
+ vector v_hi_inv = vec_reciprocal(v_hi);
+
+ /* Reset cumulative sums of update vectors. */
+ vector v_a_hydro_xSum = vector_setzero();
+ vector v_a_hydro_ySum = vector_setzero();
+ vector v_a_hydro_zSum = vector_setzero();
+ vector v_h_dtSum = vector_setzero();
+ vector v_sigSum = vector_set1(pi->force.v_sig);
+ vector v_entropy_dtSum = vector_setzero();
+
+ /* Pad the exit iteration if there is a serial remainder. */
+ int exit_iteration_align = exit_iteration;
+ const int rem = exit_iteration % VEC_SIZE;
+ if (rem != 0) {
+ int pad = VEC_SIZE - rem;
+
+ if (exit_iteration_align + pad <= last_pj + 1)
+ exit_iteration_align += pad;
+ }
+
+ /* Loop over the parts in cj. Making sure to perform an iteration of the
+ * loop even if exit_iteration_align is zero and there is only one
+ * particle to interact with.*/
+ for (int pjd = 0; pjd <= exit_iteration_align; pjd += VEC_SIZE) {
+
+ /* Get the cache index to the jth particle. */
+ const int cj_cache_idx = pjd;
+
+ vector v_dx, v_dy, v_dz, v_r2;
+ vector v_hjg2;
+
+#ifdef SWIFT_DEBUG_CHECKS
+ if (cj_cache_idx % VEC_SIZE != 0 || cj_cache_idx < 0 ||
+ cj_cache_idx + (VEC_SIZE - 1) > (last_pj + 1 + VEC_SIZE)) {
+ error("Unaligned read!!! cj_cache_idx=%d, last_pj=%d", cj_cache_idx,
+ last_pj);
+ }
+#endif
+
+ /* Load 2 sets of vectors from the particle cache. */
+ const vector v_pjx = vector_load(&cj_cache->x[cj_cache_idx]);
+ const vector v_pjy = vector_load(&cj_cache->y[cj_cache_idx]);
+ const vector v_pjz = vector_load(&cj_cache->z[cj_cache_idx]);
+ const vector v_hj = vector_load(&cj_cache->h[cj_cache_idx]);
+ v_hjg2.v = vec_mul(vec_mul(v_hj.v, v_hj.v), kernel_gamma2_vec.v);
+
+ /* Compute the pairwise distance. */
+ v_dx.v = vec_sub(v_pix.v, v_pjx.v);
+ v_dy.v = vec_sub(v_piy.v, v_pjy.v);
+ v_dz.v = vec_sub(v_piz.v, v_pjz.v);
+
+ v_r2.v = vec_mul(v_dx.v, v_dx.v);
+ v_r2.v = vec_fma(v_dy.v, v_dy.v, v_r2.v);
+ v_r2.v = vec_fma(v_dz.v, v_dz.v, v_r2.v);
+
+ mask_t v_doi_mask;
+
+ /* Form a mask from r2 < hig2 mask and r2 < hjg2 mask. */
+ vector v_h2;
+ v_h2.v = vec_fmax(v_hig2.v, v_hjg2.v);
+ vec_create_mask(v_doi_mask, vec_cmp_lt(v_r2.v, v_h2.v));
+
+ /* If there are any interactions perform them. */
+ if (vec_is_mask_true(v_doi_mask)) {
+ vector v_hj_inv = vec_reciprocal(v_hj);
+
+ runner_iact_nonsym_1_vec_force(
+ &v_r2, &v_dx, &v_dy, &v_dz, v_vix, v_viy, v_viz, v_rhoi,
+ v_grad_hi, v_pOrhoi2, v_balsara_i, v_ci,
+ &cj_cache->vx[cj_cache_idx], &cj_cache->vy[cj_cache_idx],
+ &cj_cache->vz[cj_cache_idx], &cj_cache->rho[cj_cache_idx],
+ &cj_cache->grad_h[cj_cache_idx], &cj_cache->pOrho2[cj_cache_idx],
+ &cj_cache->balsara[cj_cache_idx],
+ &cj_cache->soundspeed[cj_cache_idx], &cj_cache->m[cj_cache_idx],
+ v_hi_inv, v_hj_inv, &v_a_hydro_xSum, &v_a_hydro_ySum,
+ &v_a_hydro_zSum, &v_h_dtSum, &v_sigSum, &v_entropy_dtSum,
+ v_doi_mask);
+ }
+
+ } /* loop over the parts in cj. */
+
+ /* Perform horizontal adds on vector sums and store result in pi. */
+ VEC_HADD(v_a_hydro_xSum, pi->a_hydro[0]);
+ VEC_HADD(v_a_hydro_ySum, pi->a_hydro[1]);
+ VEC_HADD(v_a_hydro_zSum, pi->a_hydro[2]);
+ VEC_HADD(v_h_dtSum, pi->force.h_dt);
+ VEC_HMAX(v_sigSum, pi->force.v_sig);
+ VEC_HADD(v_entropy_dtSum, pi->entropy_dt);
+
+ } /* loop over the parts in ci. */
+ }
+
+ if (active_cj) {
+
+ /* Loop over the parts in cj until nothing is within range in ci. */
+ for (int pjd = 0; pjd <= last_pj_loop; pjd++) {
+
+ /* Get a hold of the jth part in cj. */
+ struct part *restrict pj = &parts_j[sort_j[pjd].i];
+ if (!part_is_active(pj, e)) continue;
+
+ /* Set the cache index. */
+ const int cj_cache_idx = pjd;
+
+ /* Skip this particle if no particle in ci is within range of it. */
+ const float hj = cj_cache->h[cj_cache_idx];
+ const double dj_test =
+ sort_j[pjd].d - max(hj, hi_max_raw) * kernel_gamma - dx_max;
+ if (dj_test > di_max) continue;
+
+ /* Determine the exit iteration of the interaction loop. */
+ const int exit_iteration = max_index_j[pjd];
+
+ /* Fill particle pi vectors. */
+ const vector v_pjx = vector_set1(cj_cache->x[cj_cache_idx]);
+ const vector v_pjy = vector_set1(cj_cache->y[cj_cache_idx]);
+ const vector v_pjz = vector_set1(cj_cache->z[cj_cache_idx]);
+ const vector v_hj = vector_set1(hj);
+ const vector v_vjx = vector_set1(cj_cache->vx[cj_cache_idx]);
+ const vector v_vjy = vector_set1(cj_cache->vy[cj_cache_idx]);
+ const vector v_vjz = vector_set1(cj_cache->vz[cj_cache_idx]);
+ const vector v_rhoj = vector_set1(cj_cache->rho[cj_cache_idx]);
+ const vector v_grad_hj = vector_set1(cj_cache->grad_h[cj_cache_idx]);
+ const vector v_pOrhoj2 = vector_set1(cj_cache->pOrho2[cj_cache_idx]);
+ const vector v_balsara_j = vector_set1(cj_cache->balsara[cj_cache_idx]);
+ const vector v_cj = vector_set1(cj_cache->soundspeed[cj_cache_idx]);
+
+ const float hjg2 = hj * hj * kernel_gamma2;
+ const vector v_hjg2 = vector_set1(hjg2);
+
+ /* Get the inverse of hj. */
+ vector v_hj_inv = vec_reciprocal(v_hj);
+
+ /* Reset cumulative sums of update vectors. */
+ vector v_a_hydro_xSum = vector_setzero();
+ vector v_a_hydro_ySum = vector_setzero();
+ vector v_a_hydro_zSum = vector_setzero();
+ vector v_h_dtSum = vector_setzero();
+ vector v_sigSum = vector_set1(pj->force.v_sig);
+ vector v_entropy_dtSum = vector_setzero();
+
+ /* Convert exit iteration to cache indices. */
+ int exit_iteration_align = exit_iteration - first_pi;
+
+ /* Pad the exit iteration align so cache reads are aligned. */
+ const int rem = exit_iteration_align % VEC_SIZE;
+ if (exit_iteration_align < VEC_SIZE) {
+ exit_iteration_align = 0;
+ } else
+ exit_iteration_align -= rem;
+
+ /* Loop over the parts in ci. */
+ for (int ci_cache_idx = exit_iteration_align;
+ ci_cache_idx < ci_cache_count; ci_cache_idx += VEC_SIZE) {
+
+#ifdef SWIFT_DEBUG_CHECKS
+ if (ci_cache_idx % VEC_SIZE != 0 || ci_cache_idx < 0) {
+ error("Unaligned read!!! ci_cache_idx=%d", ci_cache_idx);
+ }
+#endif
+
+ vector v_hig2;
+ vector v_dx, v_dy, v_dz, v_r2;
+
+ /* Load 2 sets of vectors from the particle cache. */
+ const vector v_pix = vector_load(&ci_cache->x[ci_cache_idx]);
+ const vector v_piy = vector_load(&ci_cache->y[ci_cache_idx]);
+ const vector v_piz = vector_load(&ci_cache->z[ci_cache_idx]);
+ const vector v_hi = vector_load(&ci_cache->h[ci_cache_idx]);
+ v_hig2.v = vec_mul(vec_mul(v_hi.v, v_hi.v), kernel_gamma2_vec.v);
+
+ /* Compute the pairwise distance. */
+ v_dx.v = vec_sub(v_pjx.v, v_pix.v);
+ v_dy.v = vec_sub(v_pjy.v, v_piy.v);
+ v_dz.v = vec_sub(v_pjz.v, v_piz.v);
+
+ v_r2.v = vec_mul(v_dx.v, v_dx.v);
+ v_r2.v = vec_fma(v_dy.v, v_dy.v, v_r2.v);
+ v_r2.v = vec_fma(v_dz.v, v_dz.v, v_r2.v);
+
+ mask_t v_doj_mask;
+
+ /* Form a mask from r2 < hig2 mask and r2 < hjg2 mask. */
+ vector v_h2;
+ v_h2.v = vec_fmax(v_hjg2.v, v_hig2.v);
+ vec_create_mask(v_doj_mask, vec_cmp_lt(v_r2.v, v_h2.v));
+
+ /* If there are any interactions perform them. */
+ if (vec_is_mask_true(v_doj_mask)) {
+ vector v_hi_inv = vec_reciprocal(v_hi);
+
+ runner_iact_nonsym_1_vec_force(
+ &v_r2, &v_dx, &v_dy, &v_dz, v_vjx, v_vjy, v_vjz, v_rhoj,
+ v_grad_hj, v_pOrhoj2, v_balsara_j, v_cj,
+ &ci_cache->vx[ci_cache_idx], &ci_cache->vy[ci_cache_idx],
+ &ci_cache->vz[ci_cache_idx], &ci_cache->rho[ci_cache_idx],
+ &ci_cache->grad_h[ci_cache_idx], &ci_cache->pOrho2[ci_cache_idx],
+ &ci_cache->balsara[ci_cache_idx],
+ &ci_cache->soundspeed[ci_cache_idx], &ci_cache->m[ci_cache_idx],
+ v_hj_inv, v_hi_inv, &v_a_hydro_xSum, &v_a_hydro_ySum,
+ &v_a_hydro_zSum, &v_h_dtSum, &v_sigSum, &v_entropy_dtSum,
+ v_doj_mask);
+ }
+ } /* loop over the parts in ci. */
+
+ /* Perform horizontal adds on vector sums and store result in pj. */
+ VEC_HADD(v_a_hydro_xSum, pj->a_hydro[0]);
+ VEC_HADD(v_a_hydro_ySum, pj->a_hydro[1]);
+ VEC_HADD(v_a_hydro_zSum, pj->a_hydro[2]);
+ VEC_HADD(v_h_dtSum, pj->force.h_dt);
+ VEC_HMAX(v_sigSum, pj->force.v_sig);
+ VEC_HADD(v_entropy_dtSum, pj->entropy_dt);
+
+ } /* loop over the parts in cj. */
+
+ TIMER_TOC(timer_dopair_density);
+ }
+
+#endif /* WITH_VECTORIZATION */
+}
diff --git a/src/runner_doiact_vec.h b/src/runner_doiact_vec.h
index 09dc76ef04df5d29ea32f4af24efdc09e433aa73..9d60c75b9545bfbee8023224e34d16d362560a3f 100644
--- a/src/runner_doiact_vec.h
+++ b/src/runner_doiact_vec.h
@@ -39,5 +39,8 @@ void runner_doself2_force_vec(struct runner *r, struct cell *restrict c);
void runner_dopair1_density_vec(struct runner *r, struct cell *restrict ci,
struct cell *restrict cj, const int sid,
const double *shift);
+void runner_dopair2_force_vec(struct runner *r, struct cell *restrict ci,
+ struct cell *restrict cj, const int sid,
+ const double *shift);
#endif /* SWIFT_RUNNER_VEC_H */
diff --git a/src/scheduler.c b/src/scheduler.c
index b2466d55104dbb68d7efed008af1290c4fd73212..ea2c6bde010dd387b355e961903411c0b18a41bf 100644
--- a/src/scheduler.c
+++ b/src/scheduler.c
@@ -1038,6 +1038,12 @@ void scheduler_reweight(struct scheduler *s, int verbose) {
case task_type_timestep:
cost = wscale * t->ci->count;
break;
+ case task_type_send:
+ cost = 10 * wscale * t->ci->count * t->ci->count;
+ break;
+ case task_type_recv:
+ cost = 5 * wscale * t->ci->count * t->ci->count;
+ break;
default:
cost = 0;
break;
@@ -1603,7 +1609,7 @@ void scheduler_print_tasks(const struct scheduler *s, const char *fileName) {
for (int k = nr_tasks - 1; k >= 0; k--) {
t = &tasks[tid[k]];
- if (!((1 << t->type)) || t->skip) continue;
+ if (t->skip) continue;
fprintf(file, "%d %s %s %d %d\n", k, taskID_names[t->type],
subtaskID_names[t->subtype], t->nr_unlock_tasks, t->wait);
}
diff --git a/src/tools.c b/src/tools.c
index 3ee55db3d5f5348699372d2620b6d15af38b23d0..89d89e62ea092ba6c6ec661e423d3e0ee44eb7fe 100644
--- a/src/tools.c
+++ b/src/tools.c
@@ -254,6 +254,7 @@ void pairs_all_force(struct runner *r, struct cell *ci, struct cell *cj) {
float r2, hi, hj, hig2, hjg2, dx[3];
struct part *pi, *pj;
const double dim[3] = {r->e->s->dim[0], r->e->s->dim[1], r->e->s->dim[2]};
+ const struct engine *e = r->e;
/* Implements a double-for loop and checks every interaction */
for (int i = 0; i < ci->count; ++i) {
@@ -262,6 +263,9 @@ void pairs_all_force(struct runner *r, struct cell *ci, struct cell *cj) {
hi = pi->h;
hig2 = hi * hi * kernel_gamma2;
+ /* Skip inactive particles. */
+ if (!part_is_active(pi, e)) continue;
+
for (int j = 0; j < cj->count; ++j) {
pj = &cj->parts[j];
@@ -292,6 +296,9 @@ void pairs_all_force(struct runner *r, struct cell *ci, struct cell *cj) {
hj = pj->h;
hjg2 = hj * hj * kernel_gamma2;
+ /* Skip inactive particles. */
+ if (!part_is_active(pj, e)) continue;
+
for (int i = 0; i < ci->count; ++i) {
pi = &ci->parts[i];
@@ -510,9 +517,7 @@ void shuffle_particles(struct part *parts, const int count) {
parts[i] = particle;
}
-
- } else
- error("Array not big enough to shuffle!");
+ }
}
/**
diff --git a/src/vector.h b/src/vector.h
index 3222a8a9b6a1bf7f5dc02e914a168d7c5c911b68..15a246d9b6a4d991638f7eb801e6173d977b1273 100644
--- a/src/vector.h
+++ b/src/vector.h
@@ -20,9 +20,6 @@
#ifndef SWIFT_VECTOR_H
#define SWIFT_VECTOR_H
-/* Have I already read this file? */
-#ifndef VEC_MACRO
-
/* Config parameters. */
#include "../config.h"
@@ -84,7 +81,7 @@
#define vec_cmp_lte(a, b) _mm512_cmp_ps_mask(a, b, _CMP_LE_OQ)
#define vec_cmp_gte(a, b) _mm512_cmp_ps_mask(a, b, _CMP_GE_OQ)
#define vec_cmp_result(a) ({ a; })
-#define vec_form_int_mask(a) ({ a; })
+#define vec_is_mask_true(a) ({ a; })
#define vec_and(a, b) _mm512_and_ps(a, b)
#define vec_mask_and(a, b) _mm512_kand(a, b)
#define vec_and_mask(a, mask) _mm512_maskz_mov_ps(mask, a)
@@ -182,7 +179,7 @@
#define vec_cmp_lte(a, b) _mm256_cmp_ps(a, b, _CMP_LE_OQ)
#define vec_cmp_gte(a, b) _mm256_cmp_ps(a, b, _CMP_GE_OQ)
#define vec_cmp_result(a) _mm256_movemask_ps(a)
-#define vec_form_int_mask(a) _mm256_movemask_ps(a.v)
+#define vec_is_mask_true(a) _mm256_movemask_ps(a.v)
#define vec_and(a, b) _mm256_and_ps(a, b)
#define vec_mask_and(a, b) _mm256_and_ps(a.v, b.v)
#define vec_and_mask(a, mask) _mm256_and_ps(a, mask.v)
@@ -431,11 +428,48 @@ __attribute__((always_inline)) INLINE vector vec_reciprocal_sqrt(vector x) {
return x_inv;
}
+/**
+ * @brief Returns a new vector with data loaded from a memory address.
+ *
+ * @param x memory address to load from.
+ * @return Loaded #vector.
+ */
+__attribute__((always_inline)) INLINE vector vector_load(float *const x) {
+
+ vector temp;
+ temp.v = vec_load(x);
+ return temp;
+}
+
+/**
+ * @brief Returns a vector filled with one value.
+ *
+ * @param x value to set each element.
+ * @return A #vector filled with a given constant.
+ */
+__attribute__((always_inline)) INLINE vector vector_set1(const float x) {
+
+ vector temp;
+ temp.v = vec_set1(x);
+ return temp;
+}
+
+/**
+ * @brief Returns a new vector filled with zeros.
+ *
+ * @return temp set #vector.
+ * @return A #vector filled with zeros.
+ */
+__attribute__((always_inline)) INLINE vector vector_setzero() {
+
+ vector temp;
+ temp.v = vec_setzero();
+ return temp;
+}
+
#else
/* Needed for cache alignment. */
#define VEC_SIZE 8
#endif /* WITH_VECTORIZATION */
-#endif /* VEC_MACRO */
-
#endif /* SWIFT_VECTOR_H */
diff --git a/tests/Makefile.am b/tests/Makefile.am
index 553980a93e907e83b65bb4539ca49c8bc1b7207b..f6f88b51cbdc5a7c5ab1d331b295418af66ade53 100644
--- a/tests/Makefile.am
+++ b/tests/Makefile.am
@@ -102,5 +102,5 @@ EXTRA_DIST = testReading.sh makeInput.py testActivePair.sh \
testPeriodicBCPerturbed.sh test125cells.sh test125cellsPerturbed.sh testParserInput.yaml \
difffloat.py tolerance_125_normal.dat tolerance_125_perturbed.dat \
tolerance_27_normal.dat tolerance_27_perturbed.dat tolerance_27_perturbed_h.dat tolerance_27_perturbed_h2.dat \
- tolerance_testInteractions.dat tolerance_pair_active.dat \
+ tolerance_testInteractions.dat tolerance_pair_active.dat tolerance_pair_force_active.dat \
fft_params.yml tolerance_periodic_BC_normal.dat tolerance_periodic_BC_perturbed.dat
diff --git a/tests/test125cells.c b/tests/test125cells.c
index 7a9f02d1b28fa7fa9e40d5f408001b671d54999a..bf1c219fab9927b81bb087684f6ad0d747e958bc 100644
--- a/tests/test125cells.c
+++ b/tests/test125cells.c
@@ -33,13 +33,18 @@
#if defined(WITH_VECTORIZATION)
#define DOSELF2 runner_doself2_force_vec
+#define DOPAIR2 runner_dopair2_branch_force
#define DOSELF2_NAME "runner_doself2_force_vec"
-#define DOPAIR2_NAME "runner_dopair2_force"
+#define DOPAIR2_NAME "runner_dopair2_force_vec"
#endif
#ifndef DOSELF2
#define DOSELF2 runner_doself2_force
#define DOSELF2_NAME "runner_doself2_density"
+#endif
+
+#ifndef DOPAIR2
+#define DOPAIR2 runner_dopair2_branch_force
#define DOPAIR2_NAME "runner_dopair2_force"
#endif
@@ -445,11 +450,11 @@ void dump_particle_fields(char *fileName, struct cell *main_cell,
}
/* Just a forward declaration... */
-void runner_dopair1_density(struct runner *r, struct cell *ci, struct cell *cj);
void runner_dopair1_branch_density(struct runner *r, struct cell *ci,
struct cell *cj);
void runner_doself1_density(struct runner *r, struct cell *ci);
-void runner_dopair2_force(struct runner *r, struct cell *ci, struct cell *cj);
+void runner_dopair2_branch_force(struct runner *r, struct cell *ci,
+ struct cell *cj);
void runner_doself2_force(struct runner *r, struct cell *ci);
void runner_doself2_force_vec(struct runner *r, struct cell *ci);
@@ -627,7 +632,6 @@ int main(int argc, char *argv[]) {
/* Start the test */
ticks time = 0;
- ticks self_force_time = 0;
for (size_t n = 0; n < runs; ++n) {
const ticks tic = getticks();
@@ -698,6 +702,14 @@ int main(int argc, char *argv[]) {
/* Do the force calculation */
#if !(defined(MINIMAL_SPH) && defined(WITH_VECTORIZATION))
+#ifdef WITH_VECTORIZATION
+ /* Initialise the cache. */
+ runner.ci_cache.count = 0;
+ runner.cj_cache.count = 0;
+ cache_init(&runner.ci_cache, 512);
+ cache_init(&runner.cj_cache, 512);
+#endif
+
int ctr = 0;
/* Do the pairs (for the central 27 cells) */
for (int i = 1; i < 4; i++) {
@@ -710,27 +722,19 @@ int main(int argc, char *argv[]) {
const ticks sub_tic = getticks();
- runner_dopair2_force(&runner, main_cell, cj);
+ DOPAIR2(&runner, main_cell, cj);
- const ticks sub_toc = getticks();
- timings[ctr++] += sub_toc - sub_tic;
+ timings[ctr++] += getticks() - sub_tic;
}
}
}
}
-#ifdef WITH_VECTORIZATION
- /* Initialise the cache. */
- runner.ci_cache.count = 0;
- cache_init(&runner.ci_cache, 512);
-#endif
-
ticks self_tic = getticks();
/* And now the self-interaction for the main cell */
DOSELF2(&runner, main_cell);
- self_force_time += getticks() - self_tic;
timings[26] += getticks() - self_tic;
#endif
@@ -763,11 +767,12 @@ int main(int argc, char *argv[]) {
ticks face_time = timings[4] + timings[10] + timings[12] + timings[13] +
timings[15] + timings[21];
+ ticks self_time = timings[26];
+
message("Corner calculations took : %15lli ticks.", corner_time / runs);
message("Edge calculations took : %15lli ticks.", edge_time / runs);
message("Face calculations took : %15lli ticks.", face_time / runs);
- message("Self calculations took : %15lli ticks.",
- self_force_time / runs);
+ message("Self calculations took : %15lli ticks.", self_time / runs);
message("SWIFT calculation took : %15lli ticks.", time / runs);
for (int j = 0; j < 125; ++j)
diff --git a/tests/testActivePair.c b/tests/testActivePair.c
index 1fb6b4348119d6af88e0f2175a6ea0a68c4ea873..fd2244db971f6a5f7cfeb62b9661c33b7ee88145 100644
--- a/tests/testActivePair.c
+++ b/tests/testActivePair.c
@@ -29,6 +29,9 @@
/* Local headers. */
#include "swift.h"
+/* Typdef function pointer for interaction function. */
+typedef void (*interaction_func)(struct runner *, struct cell *, struct cell *);
+
/**
* @brief Constructs a cell and all of its particle in a valid state prior to
* a DOPAIR or DOSELF calcuation.
@@ -108,6 +111,12 @@ struct cell *make_cell(size_t n, double *offset, double size, double h,
else
part->time_bin = num_time_bins + 1;
+ part->rho = 1.f;
+ part->force.f = 1.f;
+ part->force.P_over_rho2 = 1.f;
+ part->force.balsara = 1.f;
+ part->force.soundspeed = 1.f;
+
#ifdef SWIFT_DEBUG_CHECKS
part->ti_drift = 8;
part->ti_kick = 8;
@@ -133,7 +142,7 @@ struct cell *make_cell(size_t n, double *offset, double size, double h,
cell->ti_old_part = 8;
cell->ti_end_min = 8;
- cell->ti_end_max = 8;
+ cell->ti_end_max = 10;
shuffle_particles(cell->parts, cell->count);
@@ -156,6 +165,11 @@ void clean_up(struct cell *ci) {
void zero_particle_fields(struct cell *c) {
for (int pid = 0; pid < c->count; pid++) {
hydro_init_part(&c->parts[pid], NULL);
+ c->parts[pid].rho = 1.f;
+ c->parts[pid].force.f = 1.f;
+ c->parts[pid].force.P_over_rho2 = 1.f;
+ c->parts[pid].force.balsara = 1.f;
+ c->parts[pid].force.soundspeed = 1.f;
}
}
@@ -179,20 +193,20 @@ void dump_particle_fields(char *fileName, struct cell *ci, struct cell *cj) {
FILE *file = fopen(fileName, "a");
/* Write header */
- fprintf(file, "# %4s %13s\n", "ID", "wcount");
+ fprintf(file, "# %4s %13s %13s\n", "ID", "wcount", "h_dt");
fprintf(file, "# ci --------------------------------------------\n");
for (int pid = 0; pid < ci->count; pid++) {
- fprintf(file, "%6llu %13e\n", ci->parts[pid].id,
- ci->parts[pid].density.wcount);
+ fprintf(file, "%6llu %13e %13e\n", ci->parts[pid].id,
+ ci->parts[pid].density.wcount, ci->parts[pid].force.h_dt);
}
fprintf(file, "# cj --------------------------------------------\n");
for (int pjd = 0; pjd < cj->count; pjd++) {
- fprintf(file, "%6llu %13e\n", cj->parts[pjd].id,
- cj->parts[pjd].density.wcount);
+ fprintf(file, "%6llu %13e %13e\n", cj->parts[pjd].id,
+ cj->parts[pjd].density.wcount, cj->parts[pjd].force.h_dt);
}
fclose(file);
@@ -200,9 +214,13 @@ void dump_particle_fields(char *fileName, struct cell *ci, struct cell *cj) {
/* Just a forward declaration... */
void runner_dopair1_density(struct runner *r, struct cell *ci, struct cell *cj);
+void runner_dopair2_force_vec(struct runner *r, struct cell *ci,
+ struct cell *cj);
void runner_doself1_density_vec(struct runner *r, struct cell *ci);
void runner_dopair1_branch_density(struct runner *r, struct cell *ci,
struct cell *cj);
+void runner_dopair2_branch_force(struct runner *r, struct cell *ci,
+ struct cell *cj);
/**
* @brief Computes the pair interactions of two cells using SWIFT and a brute
@@ -210,7 +228,9 @@ void runner_dopair1_branch_density(struct runner *r, struct cell *ci,
*/
void test_pair_interactions(struct runner *runner, struct cell **ci,
struct cell **cj, char *swiftOutputFileName,
- char *bruteForceOutputFileName) {
+ char *bruteForceOutputFileName,
+ interaction_func serial_interaction,
+ interaction_func vec_interaction) {
runner_do_sort(runner, *ci, 0x1FFF, 0, 0);
runner_do_sort(runner, *cj, 0x1FFF, 0, 0);
@@ -220,7 +240,7 @@ void test_pair_interactions(struct runner *runner, struct cell **ci,
zero_particle_fields(*cj);
/* Run the test */
- runner_dopair1_branch_density(runner, *ci, *cj);
+ vec_interaction(runner, *ci, *cj);
/* Let's get physical ! */
end_calculation(*ci);
@@ -236,7 +256,7 @@ void test_pair_interactions(struct runner *runner, struct cell **ci,
zero_particle_fields(*cj);
/* Run the brute-force test */
- pairs_all_density(runner, *ci, *cj);
+ serial_interaction(runner, *ci, *cj);
/* Let's get physical ! */
end_calculation(*ci);
@@ -248,16 +268,26 @@ void test_pair_interactions(struct runner *runner, struct cell **ci,
/**
* @brief Computes the pair interactions of two cells in various configurations.
*/
-void test_all_pair_interactions(struct runner *runner, double *offset2,
- size_t particles, double size, double h,
- double rho, long long *partId,
- double perturbation, double h_pert,
- char *swiftOutputFileName,
- char *bruteForceOutputFileName) {
+void test_all_pair_interactions(
+ struct runner *runner, double *offset2, size_t particles, double size,
+ double h, double rho, long long *partId, double perturbation, double h_pert,
+ char *swiftOutputFileName, char *bruteForceOutputFileName,
+ interaction_func serial_interaction, interaction_func vec_interaction) {
double offset1[3] = {0, 0, 0};
struct cell *ci, *cj;
+ /* Only one particle in each cell. */
+ ci = make_cell(1, offset1, size, h, rho, partId, perturbation, h_pert, 1.);
+ cj = make_cell(1, offset2, size, h, rho, partId, perturbation, h_pert, 1.);
+
+ test_pair_interactions(runner, &ci, &cj, swiftOutputFileName,
+ bruteForceOutputFileName, serial_interaction,
+ vec_interaction);
+
+ clean_up(ci);
+ clean_up(cj);
+
/* All active particles. */
ci = make_cell(particles, offset1, size, h, rho, partId, perturbation, h_pert,
1.);
@@ -265,7 +295,8 @@ void test_all_pair_interactions(struct runner *runner, double *offset2,
1.);
test_pair_interactions(runner, &ci, &cj, swiftOutputFileName,
- bruteForceOutputFileName);
+ bruteForceOutputFileName, serial_interaction,
+ vec_interaction);
clean_up(ci);
clean_up(cj);
@@ -277,7 +308,8 @@ void test_all_pair_interactions(struct runner *runner, double *offset2,
0.5);
test_pair_interactions(runner, &ci, &cj, swiftOutputFileName,
- bruteForceOutputFileName);
+ bruteForceOutputFileName, serial_interaction,
+ vec_interaction);
clean_up(ci);
clean_up(cj);
@@ -289,7 +321,8 @@ void test_all_pair_interactions(struct runner *runner, double *offset2,
0.);
test_pair_interactions(runner, &ci, &cj, swiftOutputFileName,
- bruteForceOutputFileName);
+ bruteForceOutputFileName, serial_interaction,
+ vec_interaction);
clean_up(ci);
clean_up(cj);
@@ -301,7 +334,8 @@ void test_all_pair_interactions(struct runner *runner, double *offset2,
0.1);
test_pair_interactions(runner, &ci, &cj, swiftOutputFileName,
- bruteForceOutputFileName);
+ bruteForceOutputFileName, serial_interaction,
+ vec_interaction);
clean_up(ci);
clean_up(cj);
@@ -313,7 +347,8 @@ void test_all_pair_interactions(struct runner *runner, double *offset2,
0.);
test_pair_interactions(runner, &ci, &cj, swiftOutputFileName,
- bruteForceOutputFileName);
+ bruteForceOutputFileName, serial_interaction,
+ vec_interaction);
clean_up(ci);
clean_up(cj);
@@ -325,7 +360,8 @@ void test_all_pair_interactions(struct runner *runner, double *offset2,
1.0);
test_pair_interactions(runner, &ci, &cj, swiftOutputFileName,
- bruteForceOutputFileName);
+ bruteForceOutputFileName, serial_interaction,
+ vec_interaction);
clean_up(ci);
clean_up(cj);
@@ -335,7 +371,8 @@ void test_all_pair_interactions(struct runner *runner, double *offset2,
cj = make_cell(2, offset2, size, h, rho, partId, perturbation, h_pert, 1.0);
test_pair_interactions(runner, &ci, &cj, swiftOutputFileName,
- bruteForceOutputFileName);
+ bruteForceOutputFileName, serial_interaction,
+ vec_interaction);
clean_up(ci);
clean_up(cj);
@@ -345,7 +382,8 @@ void test_all_pair_interactions(struct runner *runner, double *offset2,
cj = make_cell(3, offset2, size, h, rho, partId, perturbation, h_pert, 0.75);
test_pair_interactions(runner, &ci, &cj, swiftOutputFileName,
- bruteForceOutputFileName);
+ bruteForceOutputFileName, serial_interaction,
+ vec_interaction);
clean_up(ci);
clean_up(cj);
@@ -357,7 +395,8 @@ void test_all_pair_interactions(struct runner *runner, double *offset2,
0.);
test_pair_interactions(runner, &ci, &cj, swiftOutputFileName,
- bruteForceOutputFileName);
+ bruteForceOutputFileName, serial_interaction,
+ vec_interaction);
clean_up(ci);
clean_up(cj);
@@ -369,7 +408,8 @@ void test_all_pair_interactions(struct runner *runner, double *offset2,
0.5);
test_pair_interactions(runner, &ci, &cj, swiftOutputFileName,
- bruteForceOutputFileName);
+ bruteForceOutputFileName, serial_interaction,
+ vec_interaction);
/* Clean things to make the sanitizer happy ... */
clean_up(ci);
@@ -472,7 +512,7 @@ int main(int argc, char *argv[]) {
/* Create output file names. */
sprintf(swiftOutputFileName, "swift_dopair_%s.dat", outputFileNameExtension);
- sprintf(bruteForceOutputFileName, "brute_force_%s.dat",
+ sprintf(bruteForceOutputFileName, "brute_force_pair_%s.dat",
outputFileNameExtension);
/* Delete files if they already exist. */
@@ -488,10 +528,56 @@ int main(int argc, char *argv[]) {
double offset[3] = {1., 0., 0.};
+ /* Define which interactions to call */
+ interaction_func serial_inter_func = &pairs_all_density;
+ interaction_func vec_inter_func = &runner_dopair1_branch_density;
+
/* Test a pair of cells face-on. */
test_all_pair_interactions(runner, offset, particles, size, h, rho, &partId,
perturbation, h_pert, swiftOutputFileName,
- bruteForceOutputFileName);
+ bruteForceOutputFileName, serial_inter_func,
+ vec_inter_func);
+
+ /* Test a pair of cells edge-on. */
+ offset[0] = 1.;
+ offset[1] = 1.;
+ offset[2] = 0.;
+ test_all_pair_interactions(runner, offset, particles, size, h, rho, &partId,
+ perturbation, h_pert, swiftOutputFileName,
+ bruteForceOutputFileName, serial_inter_func,
+ vec_inter_func);
+
+ /* Test a pair of cells corner-on. */
+ offset[0] = 1.;
+ offset[1] = 1.;
+ offset[2] = 1.;
+ test_all_pair_interactions(runner, offset, particles, size, h, rho, &partId,
+ perturbation, h_pert, swiftOutputFileName,
+ bruteForceOutputFileName, serial_inter_func,
+ vec_inter_func);
+
+ /* Re-assign function pointers. */
+ serial_inter_func = &pairs_all_force;
+ vec_inter_func = &runner_dopair2_branch_force;
+
+ /* Create new output file names. */
+ sprintf(swiftOutputFileName, "swift_dopair2_force_%s.dat",
+ outputFileNameExtension);
+ sprintf(bruteForceOutputFileName, "brute_force_dopair2_%s.dat",
+ outputFileNameExtension);
+
+ /* Delete files if they already exist. */
+ remove(swiftOutputFileName);
+ remove(bruteForceOutputFileName);
+
+ /* Test a pair of cells face-on. */
+ offset[0] = 1.;
+ offset[1] = 0.;
+ offset[2] = 0.;
+ test_all_pair_interactions(runner, offset, particles, size, h, rho, &partId,
+ perturbation, h_pert, swiftOutputFileName,
+ bruteForceOutputFileName, serial_inter_func,
+ vec_inter_func);
/* Test a pair of cells edge-on. */
offset[0] = 1.;
@@ -499,7 +585,8 @@ int main(int argc, char *argv[]) {
offset[2] = 0.;
test_all_pair_interactions(runner, offset, particles, size, h, rho, &partId,
perturbation, h_pert, swiftOutputFileName,
- bruteForceOutputFileName);
+ bruteForceOutputFileName, serial_inter_func,
+ vec_inter_func);
/* Test a pair of cells corner-on. */
offset[0] = 1.;
@@ -507,6 +594,7 @@ int main(int argc, char *argv[]) {
offset[2] = 1.;
test_all_pair_interactions(runner, offset, particles, size, h, rho, &partId,
perturbation, h_pert, swiftOutputFileName,
- bruteForceOutputFileName);
+ bruteForceOutputFileName, serial_inter_func,
+ vec_inter_func);
return 0;
}
diff --git a/tests/testActivePair.sh.in b/tests/testActivePair.sh.in
index 108da19c5c667a6a46a81707a7508a27f39f6b38..87d09cad7118c45b41c5a41058c331cbda92b613 100755
--- a/tests/testActivePair.sh.in
+++ b/tests/testActivePair.sh.in
@@ -8,7 +8,9 @@ echo "Running ./testActivePair -n 6 -r 1 -d 0 -f active"
./testActivePair -n 6 -r 1 -d 0 -f active
-python @srcdir@/difffloat.py brute_force_active.dat swift_dopair_active.dat @srcdir@/tolerance_pair_active.dat
+python @srcdir@/difffloat.py brute_force_pair_active.dat swift_dopair_active.dat @srcdir@/tolerance_pair_active.dat
+
+python @srcdir@/difffloat.py brute_force_dopair2_active.dat swift_dopair2_force_active.dat @srcdir@/tolerance_pair_force_active.dat
rm -f brute_force_pair_active.dat swift_dopair_active.dat
@@ -17,6 +19,8 @@ echo "Running ./testActivePair -n 6 -r 1 -d 0 -f active -s 1506434777"
./testActivePair -n 6 -r 1 -d 0 -f active -s 1506434777
-python @srcdir@/difffloat.py brute_force_active.dat swift_dopair_active.dat @srcdir@/tolerance_pair_active.dat
+python @srcdir@/difffloat.py brute_force_pair_active.dat swift_dopair_active.dat @srcdir@/tolerance_pair_active.dat
+
+python @srcdir@/difffloat.py brute_force_dopair2_active.dat swift_dopair2_force_active.dat @srcdir@/tolerance_pair_force_active.dat
exit $?
diff --git a/tests/tolerance_27_perturbed_h.dat b/tests/tolerance_27_perturbed_h.dat
index e25c3373afe6f2a8e7788dfc2d9eba0b74efdbee..5d6710c3946c0515f94c58eb3e0ecbfe14135b71 100644
--- a/tests/tolerance_27_perturbed_h.dat
+++ b/tests/tolerance_27_perturbed_h.dat
@@ -1,4 +1,4 @@
# ID pos_x pos_y pos_z v_x v_y v_z rho rho_dh wcount wcount_dh div_v curl_vx curl_vy curl_vz
- 0 1e-6 1e-6 1e-6 1e-6 1e-6 1e-6 2.4e-6 1e-4 5e-4 1.2e-2 1.1e-5 3e-6 3e-6 8e-6
- 0 1e-6 1e-6 1e-6 1e-6 1e-6 1e-6 1.2e-6 1.4e-2 1e-5 2e-3 2.5e-4 3e-3 3e-3 3e-3
+ 0 1e-6 1e-6 1e-6 1e-6 1e-6 1e-6 3e-6 1e-4 5e-4 1.4e-2 1.1e-5 3e-6 3e-6 8e-6
+ 0 1e-6 1e-6 1e-6 1e-6 1e-6 1e-6 1.5e-6 1.4e-2 1e-5 2e-3 2.5e-4 3e-3 3e-3 3e-3
0 1e-6 1e-6 1e-6 1e-6 1e-6 1e-6 1e-6 1e-6 1e-6 1e0 1e-6 4e-6 4e-6 4e-6
diff --git a/tests/tolerance_27_perturbed_h2.dat b/tests/tolerance_27_perturbed_h2.dat
index d83f36a887d92b55c90b21adae65ffe734a2f188..9ae7dfe979bce3d047c810be128521de52f8a8a9 100644
--- a/tests/tolerance_27_perturbed_h2.dat
+++ b/tests/tolerance_27_perturbed_h2.dat
@@ -1,4 +1,4 @@
# ID pos_x pos_y pos_z v_x v_y v_z rho rho_dh wcount wcount_dh div_v curl_vx curl_vy curl_vz
0 1e-6 1e-6 1e-6 1e-6 1e-6 1e-6 3e-6 1e-4 5e-4 1.5e-2 1.4e-5 3e-6 3e-6 1e-5
- 0 1e-6 1e-6 1e-6 1e-6 1e-6 1e-6 1.5e-6 1.57e-2 1e-5 5.86e-3 4.96e-4 3e-3 3e-3 3e-3
+ 0 1e-6 1e-6 1e-6 1e-6 1e-6 1e-6 1.5e-6 2.5e-2 1e-5 5.86e-3 4.96e-4 3e-3 3.7e-3 3e-3
0 1e-6 1e-6 1e-6 1e-6 1e-6 1e-6 1e-6 1e-6 1e-6 1e0 1e-6 4e-6 4e-6 4e-6
diff --git a/tests/tolerance_pair_active.dat b/tests/tolerance_pair_active.dat
index b07697a686eb7801326ceaf77cf93fb3a1491c2e..087c33fb8fa73c6125231b3f58cc9412a96c771b 100644
--- a/tests/tolerance_pair_active.dat
+++ b/tests/tolerance_pair_active.dat
@@ -1,4 +1,4 @@
-# ID wcount
- 0 1e-2
- 0 1e-2
- 0 1e-2
+# ID wcount h_dt
+ 0 1e-2 1
+ 0 1e-2 1
+ 0 1e-2 1
diff --git a/tests/tolerance_pair_force_active.dat b/tests/tolerance_pair_force_active.dat
new file mode 100644
index 0000000000000000000000000000000000000000..c5b5620338b848f1b8f4658049e53a6424e93a60
--- /dev/null
+++ b/tests/tolerance_pair_force_active.dat
@@ -0,0 +1,4 @@
+# ID wcount h_dt
+ 0 1 2.4e-3
+ 0 1 2.4e-3
+ 0 1 1e-5
diff --git a/theory/Papers/Parco_2017/Figures/parts_on_axis.eps b/theory/Papers/Parco_2017/Figures/parts_on_axis.eps
new file mode 100644
index 0000000000000000000000000000000000000000..a62286f75f1f2c6cfbe4c3b7d46ff27160941261
--- /dev/null
+++ b/theory/Papers/Parco_2017/Figures/parts_on_axis.eps
@@ -0,0 +1,858 @@
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+Q
+Q Q
+showpage
+%%Trailer
+end restore
+%%EOF
diff --git a/theory/Papers/Parco_2017/IOS-Book-Article.cls b/theory/Papers/Parco_2017/IOS-Book-Article.cls
new file mode 100644
index 0000000000000000000000000000000000000000..e202f3f032cadf4cbb2ef23c22b4078e77dc59e4
--- /dev/null
+++ b/theory/Papers/Parco_2017/IOS-Book-Article.cls
@@ -0,0 +1,1200 @@
+%% This is file `IOSarticle.cls'
+%%
+%% Generic LaTeX 2e class file for the IOS Press publications
+%%
+%% Macros written by Vytas Statulevicius, VTeX, Lithuania
+%% for IOS Press, The Netherlands
+%% Please submit bugs or your comments to vytas@vtex.lt
+%%
+%% You are free to use this class file as you see fit, provided
+%% that you do not make changes to the file.
+%% If you DO make changes, you are required to rename this file.
+%%
+%% It may be distributed under the terms of the LaTeX Project Public
+%% License, as described in lppl.txt in the base LaTeX distribution.
+%% Either version 1.0 or, at your option, any later version.
+%%
+%% \CharacterTable
+%% {Upper-case \A\B\C\D\E\F\G\H\I\J\K\L\M\N\O\P\Q\R\S\T\U\V\W\X\Y\Z
+%% Lower-case \a\b\c\d\e\f\g\h\i\j\k\l\m\n\o\p\q\r\s\t\u\v\w\x\y\z
+%% Digits \0\1\2\3\4\5\6\7\8\9
+%% Exclamation \! Double quote \" Hash (number) \#
+%% Dollar \$ Percent \% Ampersand \&
+%% Acute accent \' Left paren \( Right paren \)
+%% Asterisk \* Plus \+ Comma \,
+%% Minus \- Point \. Solidus \/
+%% Colon \: Semicolon \; Less than \<
+%% Equals \= Greater than \> Question mark \?
+%% Commercial at \@ Left bracket \[ Backslash \\
+%% Right bracket \] Circumflex \^ Underscore \_
+%% Grave accent \` Left brace \{ Vertical bar \|
+%% Right brace \} Tilde \~}
+%%
+%%
+%% Bug fixes and changes:
+%% 2004.05.19 - small change o layout
+%% 2004.09.14 - \parindent changed
+%% 2006.03.27 - centering on A4, no running heads, \snm makes uppercase
+%% 2006.04.20 - changed: \thebibliography size, indent, \parindent
+
+\NeedsTeXFormat{LaTeX2e}[1995/12/01]
+\ProvidesClass{IOS-Book-Article}
+ [2006/04/20 v1.0, IOS Press]
+
+\newif\if@restonecol \@restonecolfalse
+\newif\if@openright
+\newif\if@mainmatter \@mainmattertrue
+
+\DeclareOption{draft}{\setlength\overfullrule{5pt}}
+\DeclareOption{final}{\setlength\overfullrule{0pt}}
+\DeclareOption{openright}{\@openrighttrue}
+\DeclareOption{openany}{\@openrightfalse}
+\DeclareOption{onecolumn}{\@twocolumnfalse\@restonecoltrue}
+\DeclareOption{twocolumn}{\@twocolumntrue}
+\DeclareOption{leqno}{\input{leqno.clo}}
+\DeclareOption{fleqn}{\input{fleqn.clo}}%
+%
+% Numbering switches:
+\newif\if@seceqn \@seceqnfalse \DeclareOption{seceqn}{\@seceqntrue}
+\newif\if@secfloat \@secfloatfalse \DeclareOption{secfloat}{\@secfloattrue}
+\newif\if@secthm \DeclareOption{secthm}{\@secthmtrue}
+%
+%
+% Selection of font size and page dimensions
+% If 12pt option is used, page will be reduced by 80% at printing time
+\newif\if@ten@point \@ten@pointfalse
+
+\DeclareOption{10pt}{\@ten@pointtrue}
+\DeclareOption{12pt}{\@ten@pointfalse}
+
+% Information about the publication
+\def\booktitle#1{\gdef\book@title{#1}}
+\def\bookeditors#1{\gdef\book@editors{#1}}
+\def\publisher#1{\gdef\@publisher{#1}}
+
+\booktitle{Book Title}
+\bookeditors{Book Editors}
+\publisher{IOS Press}
+
+\ExecuteOptions{10pt,onecolumn,twoside,final,openright,fleqn}
+\ProcessOptions
+%
+
+%************************* FONTS
+%\def\@xivpt{14}
+%\def\@xviipt{17}
+%\def\@xviiipt{18}
+%\def\@xxpt{20}
+%\def\@xxivpt{24}
+
+% Fonts:
+\typeout{Ten point}
+%
+\renewcommand\normalsize{%
+ \@setfontsize\normalsize\@xpt{12pt plus .5\p@ minus .1\p@}%
+ \abovedisplayskip 12\p@ \@plus3pt \@minus3pt%
+ \abovedisplayshortskip\abovedisplayskip%
+ \belowdisplayshortskip\abovedisplayskip%
+ \belowdisplayskip \abovedisplayskip%
+ \let\@listi\@listI}
+
+\newcommand\small{%
+ \@setfontsize\small\@ixpt\@xipt%
+ \abovedisplayskip 5.5\p@ \@plus3pt%
+ \abovedisplayshortskip 5.5\p@ \@plus1pt \@minus1pt%
+ \belowdisplayshortskip 5.5\p@ \@plus1pt \@minus1pt%
+ \def\@listi{\leftmargin\leftmargini
+ \topsep 5\p@ \@plus2\p@ \@minus2\p@
+ \parsep \z@ \itemsep \parsep}%
+ \belowdisplayskip \abovedisplayskip%
+}
+\newcommand\footnotesize{%
+ \@setfontsize\footnotesize\@viiipt\@xpt%
+ \abovedisplayskip 5.5\p@ \@plus3pt%
+ \abovedisplayshortskip 5.5\p@ \@plus1pt \@minus1pt%
+ \belowdisplayshortskip 5.5\p@ \@plus1pt \@minus1pt%
+ \def\@listi{\leftmargin\leftmargini
+ \topsep 4\p@ \@plus2\p@ \@minus2\p@
+ \parsep \z@ \itemsep \parsep}%
+ \belowdisplayskip \abovedisplayskip%
+}
+\newcommand\scriptsize{\@setfontsize\scriptsize\@viiipt{9.5}}
+\newcommand\tiny{\@setfontsize\tiny\@vipt\@viipt}
+\newcommand\large{\@setfontsize\large\@xiipt{14}}
+\newcommand\Large{\@setfontsize\Large\@xivpt{18}}
+\newcommand\LARGE{\@setfontsize\LARGE\@xviipt{22}}
+\newcommand\huge{\@setfontsize\huge\@xxpt{25}}
+\newcommand\Huge{\@setfontsize\Huge\@xxvpt{30}}
+
+\normalsize
+
+% Customization of fonts
+\renewcommand\sldefault{it}
+\renewcommand\bfdefault{b}
+\let\slshape\itshape
+%
+
+% ********************* DIMENSIONS:
+% TEXT DIMENSIONS
+\setlength\parindent{18\p@}
+\@settopoint\parindent
+\setlength\textwidth{124mm}
+\@settopoint\textwidth
+\setlength\textheight{200mm}
+\@settopoint\textheight
+\setlength\columnsep{10mm}
+\@settopoint\columnsep
+\setlength\columnwidth{95mm}
+\@settopoint\columnwidth
+\setlength\columnseprule{0\p@}
+\hoffset -0.5cm
+\voffset -1cm
+
+% HEADS:
+\setlength\headheight{12\p@}
+\setlength\headsep {15\p@}
+\setlength\topskip {10\p@}
+\setlength\footskip {25\p@}
+\setlength\maxdepth {.5\topskip}
+% SIDE MARGINS
+\setlength\oddsidemargin {0mm}
+\setlength\evensidemargin {0mm}
+\setlength\topmargin {10mm}
+\@settopoint\topmargin
+% TEXT PARAMETERS
+\setlength\lineskip{1\p@}
+\setlength\normallineskip{1\p@}
+\renewcommand\baselinestretch{}
+\setlength\parskip{0\p@}
+
+% Center on A4:
+
+\def\paper@width {210mm}
+\def\paper@height{297mm}
+
+\hoffset=-1in
+\voffset=-1in
+
+\@tempdima=\paper@width
+\advance\@tempdima by-\textwidth
+\divide\@tempdima by2
+\setlength\evensidemargin {\@tempdima}%
+\setlength\oddsidemargin {\@tempdima}%
+
+\@tempdima=\paper@height
+\advance\@tempdima by-\textheight
+\advance\@tempdima by-\headsep
+\advance\@tempdima by-\headheight
+\divide\@tempdima by2
+\setlength\topmargin {\@tempdima}%
+
+
+
+
+% BREAKS
+\setlength\smallskipamount{6\p@ \@plus 1\p@ \@minus 1\p@}
+\setlength\medskipamount{12\p@ \@plus 3\p@ \@minus 3\p@}
+\setlength\bigskipamount{24pt \@plus 3\p@ \@minus 3\p@}
+% PAGE-BREAKING PENALTIES
+\clubpenalty=4000
+\widowpenalty=4000
+\displaywidowpenalty=50
+\predisplaypenalty=0 % Breaking before a math display.
+% \postdisplaypenalty % Breaking after a math display.
+% \interlinepenalty % Breaking at a line within a paragraph.
+% \brokenpenalty % Breaking after a hyphenated line.
+\pretolerance=100 % Badness tolerance for the first pass (before hyphenation)
+\tolerance=800 % Badness tolerance after hyphenation
+\hbadness=800 % Badness above which bad hboxes will be shown
+\emergencystretch=3\p@
+\hfuzz=1\p@ % do not be to critical about boxes
+
+%
+\doublehyphendemerits=0
+\adjdemerits=0
+\brokenpenalty=0
+\interlinepenalty=0
+%
+\if@twocolumn
+ \setlength\marginparsep {10\p@}
+\else
+ \setlength\marginparsep{7\p@}
+\fi
+\setlength\marginparpush{5\p@}
+
+% FOOTNOTES
+\setlength\footnotesep{6.65\p@}
+\setlength{\skip\footins}{12\p@ \@plus 6\p@}
+% FLOATS
+\setlength\floatsep {15\p@ \@plus 10\p@ \@minus 4\p@}
+\setlength\textfloatsep{12\p@ \@plus 6\p@ \@minus 4\p@}
+\setlength\intextsep {12\p@ \@plus 6\p@ \@minus 4\p@}
+\setlength\dblfloatsep {15\p@ \@plus 10\p@ \@minus 4\p@}
+\setlength\dbltextfloatsep{12\p@ \@plus 12\p@ \@minus 4\p@}
+% For floats on a separate float page or column:
+\setlength\@fptop{0\p@ \@plus 1fil}
+\setlength\@fpsep{8\p@ \@plus 1000fil}
+\setlength\@fpbot{0\p@ \@plus 1fil}
+\setlength\@dblfptop{0\p@ \@plus 1fil}
+\setlength\@dblfpsep{8\p@ \@plus 1000fil}
+\setlength\@dblfpbot{0\p@ \@plus 1fil}
+%
+\setcounter{topnumber}{5}
+\renewcommand\topfraction{.90}
+\setcounter{bottomnumber}{5}
+\renewcommand\bottomfraction{.90}
+\setcounter{totalnumber}{10}
+\renewcommand\textfraction{.10}
+\renewcommand\floatpagefraction{.9}
+\setcounter{dbltopnumber}{5}
+\renewcommand\dbltopfraction{.99}
+\renewcommand\dblfloatpagefraction{.8}
+%
+% PENALTIES
+\@lowpenalty 51
+\@medpenalty 151
+\@highpenalty 301
+\@beginparpenalty -\@lowpenalty
+\@endparpenalty -\@lowpenalty
+\@itempenalty -\@lowpenalty
+% LISTS
+\setlength\partopsep{0\p@}
+\def\@listI{\leftmargin\leftmargini
+ \parsep 0\p@ \@plus2\p@ \@minus\p@
+ \topsep 9\p@ \@plus2\p@ \@minus2\p@
+ \partopsep\p@
+ \itemsep 1\p@ \@plus.5\p@ \@minus1\p@}
+\let\@listi\@listI
+\@listi
+\def\@listii {\leftmargin\leftmarginii
+ \labelwidth\leftmarginii
+ \advance\labelwidth-\labelsep
+ \topsep 4\p@ \@plus2\p@ \@minus\p@
+ \parsep 0\p@ \@plus1\p@ \@minus\p@
+ \itemsep \parsep}
+\def\@listiii{\leftmargin\leftmarginiii
+ \labelwidth\leftmarginiii
+ \advance\labelwidth-\labelsep
+ \topsep 2\p@ \@plus\p@\@minus\p@
+ \parsep \z@
+ \partopsep \p@ \@plus\z@ \@minus\p@
+ \itemsep \topsep}
+\def\@listiv {\leftmargin\leftmarginiv
+ \labelwidth\leftmarginiv
+ \advance\labelwidth-\labelsep}
+\def\@listv {\leftmargin\leftmarginv
+ \labelwidth\leftmarginv
+ \advance\labelwidth-\labelsep}
+\def\@listvi {\leftmargin\leftmarginvi
+ \labelwidth\leftmarginvi
+ \advance\labelwidth-\labelsep}
+%
+\DeclareMathSizes{\@xivpt}{\@xivpt}{\@xpt}{\@viiipt}
+\DeclareMathSizes{12}{12}{\@viiipt}{\@viipt}
+%
+% ******************** HEADINGS
+%
+% normal heading
+\def\ps@headings{%
+ \let\@oddfoot\@empty\let\@evenfoot\@empty
+ \def\@evenhead{\footnotesize\rlap{\thepage}\hfill\textit{\leftmark}\hfill}%
+ \def\@oddhead{\footnotesize\hfill\textit{\rightmark}\hfill\llap{\thepage}}%
+}%
+% empty RH
+\def\ps@empty{\let\@mkboth\@gobbletwo
+ \def\@oddhead{\hfill}\def\@oddfoot{}
+\let\@evenhead\@oddhead\let\@evenfoot\@oddfoot}
+%
+% RH with pagenumber at bottom
+\def\ps@plain{\let\@mkboth\@gobbletwo
+ \def\@oddhead{\hfill}\def\@oddfoot{}
+\let\@evenhead\@oddhead
+ \def\@oddfoot{\hfill\footnotesize\thepage\hfill}
+ \let\@evenfoot\@oddfoot
+}
+% First page RH
+\def\ps@copyright{\let\@mkboth\@gobbletwo
+ \def\@evenhead{\parbox[t]{.75\textwidth}{\footnotesize\raggedright\itshape\titleheadline}\hfill\footnotesize\thepage}%
+ \def\@oddhead {\parbox[t]{.75\textwidth}{\footnotesize\raggedright\itshape\titleheadline}\hfill\footnotesize\thepage}%
+ \let\@oddfoot\relax%
+ \let\@evenfoot\@oddfoot%
+}
+%
+% HEADLINE: Book Title
+% Book Editors
+% IOS Press, 0000
+%
+\def\titleheadline{%
+ \book@title\\
+ \book@editors\\
+ \@publisher, \the\@pubyear}
+%
+\def\@copyright{\@issn/\the@copyear/\$\@price\ \copyright@sign\
+\the\@pubyear\@copyrightowner}%
+%
+
+% ************************ FOOTNOTE
+%
+\newcommand\@makefntext[1]{%
+ \parindent1em\@makefnmark #1}
+\def\@makefnmark{\@textsuperscript{\normalfont\@thefnmark}}%
+%
+% ************************ Counters
+\setcounter{secnumdepth}{3}
+\newcounter {section}
+\newcounter {subsection}[section]
+\newcounter {subsubsection}[subsection]
+\newcounter {paragraph}[subsubsection]
+\newcounter {subparagraph}[paragraph]
+\renewcommand \thesection {\@arabic\c@section}
+\renewcommand\thesubsection {\thesection.\@arabic\c@subsection}
+\renewcommand\thesubsubsection{\thesubsection .\@arabic\c@subsubsection}
+\renewcommand\theparagraph {\thesubsubsection.\@arabic\c@paragraph}
+\renewcommand\thesubparagraph {\theparagraph.\@arabic\c@subparagraph}
+%
+% ******************** Sectioning commands
+\def\no@harm{\let\thanks=\@gobble \let\\=\@empty}
+%**************** Section commands
+\def\nohyphen{\pretolerance=10000 \tolerance=10000
+\hyphenpenalty=10000 \exhyphenpenalty=10000}
+\newcommand\section{\@startsection {section}{1}{\z@}%
+ {-\bigskipamount}%
+ {\medskipamount}%
+ {\normalsize\bfseries\nohyphen\raggedright}}
+\newcommand\subsection{\@startsection {subsection}{2}{\z@}%
+ {-\medskipamount}%
+ {\medskipamount}%
+ {\normalsize\itshape\nohyphen\raggedright}}
+\newcommand\subsubsection{\@startsection{subsubsection}{3}{\z@}%
+ {-\medskipamount}%
+ {\smallskipamount}%
+ {\normalsize\itshape\nohyphen\raggedright}}
+\newcommand\paragraph{\@startsection{paragraph}{4}{\z@}%
+ {\smallskipamount}%
+ {-1em}%
+ {\normalsize\itshape}}
+\newcommand\subparagraph{\@startsection{subparagraph}{5}{\z@}%
+ {0.1pt}%
+ {-1em}%
+ {\normalsize\itshape}}
+% Format for the counter:
+\def\@seccntformat#1{\csname the#1\endcsname.\enspace}
+%
+\def\appendix{\par
+ \setcounter{section}{0}%
+ \setcounter{subsection}{0}%
+ \gdef\thesection{\Alph{section}}}
+%
+\def\acknowledgements{\section*{\acknowledgementsname}%
+ \typeout{\acknowledgementsname}}
+%
+\def\notes{\section*{Notes}\footnotesize}
+\def\endnotes{\par \vskip 6pt plus12pt minus2pt\relax}
+%****************** LISTS
+\if@twocolumn
+ \setlength\leftmargini {2em}
+\else
+ \setlength\leftmargini {2.5em}
+\fi
+\leftmargin \leftmargini
+\setlength\leftmarginii {2.2em}
+\setlength\leftmarginiii {1.87em}
+\setlength\leftmarginiv {1.7em}
+\if@twocolumn
+ \setlength\leftmarginv {.5em}
+ \setlength\leftmarginvi {.5em}
+\else
+ \setlength\leftmarginv {1em}
+ \setlength\leftmarginvi {1em}
+\fi
+\setlength \labelsep {.4em}
+\setlength \labelwidth{\leftmargini}
+\addtolength\labelwidth{-\labelsep}
+%
+\renewcommand\theenumi{\@arabic\c@enumi}
+\renewcommand\theenumii{\@alph\c@enumii}
+\renewcommand\theenumiii{\@roman\c@enumiii}
+\renewcommand\theenumiv{\@Alph\c@enumiv}
+\newcommand\labelenumi{\theenumi.}
+\newcommand\labelenumii{(\theenumii)}
+\newcommand\labelenumiii{\theenumiii.}
+\newcommand\labelenumiv{\theenumiv.}
+\renewcommand\p@enumii{\theenumi}
+\renewcommand\p@enumiii{\theenumi(\theenumii)}
+\renewcommand\p@enumiv{\p@enumiii\theenumiii}
+%
+\def\setenumlabel#1{\gdef\max@enumlabel{#1}}
+\setenumlabel{1.}
+%
+\def\enumerate{\@ifnextchar[{\enumerate@}{\enumerate@[\max@enumlabel]}}
+%
+\def\enumerate@[#1]{\ifnum \@enumdepth >4 \@toodeep\else
+ \advance\@enumdepth \@ne
+ \edef\@enumctr{enum\romannumeral\the\@enumdepth}%
+ \list {\csname label\@enumctr\endcsname}%
+ {\usecounter{\@enumctr}\def\makelabel##1{{\hfill\rm ##1}}
+\settowidth{\labelwidth}{#1}
+\advance\labelwidth by\parindent \labelsep=0.5em
+ \leftmargin\z@ \rightmargin\z@ \itemindent=\labelwidth
+ \advance\itemindent\labelsep
+ \leftmargin=\the\itemindent\itemindent=\z@
+ \partopsep\z@ \topsep\smallskipamount \parsep\z@ \itemsep\z@ %\@rightskip\z@ plus 1fil
+ \listparindent\z@}\fi\setenumlabel{1.}}
+
+%%%%%%%%%%%%%%%%%%%%%% ITEMIZE
+\newcommand\labelitemi{\normalfont\bfseries \textbullet}
+\newcommand\labelitemii{\textasteriskcentered}
+\newcommand\labelitemiii{\textasteriskcentered}
+\newcommand\labelitemiv{\textperiodcentered}
+
+\let\@itemize@indent\parindent
+%
+\def\itemize{\@ifnextchar[{\itemize@}{\itemize@[]}}
+\def\itemize@[#1]{\ifnum \@itemdepth >4 \@toodeep\else
+ \advance\@itemdepth \@ne
+ \edef\@itemitem{labelitem\romannumeral\the\@itemdepth}%
+ \if.#1. \else\def\@@tempa{#1}\edef\@itemitem{@@tempa}\fi\list
+{\csname\@itemitem\endcsname}{\settowidth{\labelwidth}
+ {\csname\@itemitem\endcsname}
+ \def\makelabel##1{##1}\labelsep=0.5em%ST
+ \itemindent=\labelwidth \advance\itemindent\labelsep
+ \advance\itemindent\@itemize@indent
+ \leftmargin\the\itemindent \itemindent=\z@
+ \partopsep\z@ \topsep\smallskipamount \parsep\z@ %\@rightskip\z@ plus 1fil
+ \itemsep\z@ \listparindent\z@} \fi}
+%
+\newenvironment{description}
+ {\list{}{\labelwidth\z@ \itemindent-\leftmargin
+ \let\makelabel\descriptionlabel}}
+ {\endlist}
+\newcommand*\descriptionlabel[1]{\hspace\labelsep
+ \normalfont\bfseries #1}
+\newenvironment{verse}
+ {\let\\\@centercr
+ \list{}{\itemsep \z@
+ \itemindent -1.5em%
+ \listparindent\itemindent
+ \rightmargin \leftmargin
+ \advance\leftmargin 1.5em}%
+ \item\relax}
+ {\endlist}
+
+\newenvironment{quotation}
+ {\list{}{\small\listparindent2mm%
+ \itemindent\z@ %
+ \rightmargin\z@ \leftmargin\parindent%
+ \partopsep\z@ \topsep\smallskipamount \parsep\z@%
+ }%
+ \item[\Q@strut]\relax}
+ {\endlist}
+\def\Q@strut{\leavevmode\hbox{\vrule height9pt depth1pt width0pt}}
+
+\newenvironment{quote}
+ {\list{}{\listparindent\z@%
+ \itemindent \listparindent%
+ \rightmargin\z@ \leftmargin 1.5em%
+ \partopsep\z@ \topsep6pt \parsep\z@%
+ }%
+ \item[\Q@strut]\relax}
+ {\endlist}
+%
+%************************** TABULAR
+\let\savehline\hline
+ \def\thline{\noalign{\vskip3pt}\savehline\noalign{\vskip3pt}}%
+ \def\fhline{\noalign{\vskip1pt}\savehline\noalign{\vskip7pt}}%
+ \def\bhline{\noalign{\vskip3pt}\noalign{\global\arrayrulewidth=1\p@}\savehline\noalign{\global\arrayrulewidth=.5\p@}\noalign{\vskip3pt}}%
+ \def\lhline{\noalign{\vskip3pt}\noalign{\global\arrayrulewidth=.3\p@}\savehline\noalign{\global\arrayrulewidth=.5\p@}\noalign{\vskip3pt}}
+%
+%************************** MATH SETTINGS
+\setlength\mathindent{2em}
+\setlength\arraycolsep{1.2\p@}
+\setlength\tabcolsep{6\p@}
+\setlength\arrayrulewidth{.4\p@}
+\setlength\doublerulesep{2\p@}
+\setlength\tabbingsep{\labelsep}
+\setlength\jot{6\p@}
+\skip\@mpfootins = \skip\footins
+\setlength\fboxsep{3\p@}
+\setlength\fboxrule{.4\p@}
+\if@seceqn
+\@addtoreset {equation}{section}
+\renewcommand\theequation{\thesection.\@arabic\c@equation}
+\else
+\renewcommand\theequation{\@arabic\c@equation}
+\fi
+%******* TABLES, FIGURES, ALGORITHM
+\newcounter{figure}
+\if@secfloat
+ \@addtoreset{figure}{section}
+ \renewcommand \thefigure {\thesection.\@arabic\c@figure}
+\else
+ \renewcommand \thefigure {\@arabic\c@figure}
+\fi
+\def\fps@figure{tbp}
+\def\ftype@figure{1}
+\def\ext@figure{lof}
+\def\fnum@figure{\figurename~\thefigure.}
+\newenvironment{figure}
+ {\let\@makecaption\@makefigurecaption\let\@floatboxreset\@figureboxreset\@float{figure}}
+ {\end@float}
+\newenvironment{figure*}
+ {\let\@makecaption\@makefigurecaption\let\@floatboxreset\@figureboxreset\@dblfloat{figure}}
+ {\end@dblfloat}
+
+\def\@figureboxreset{%
+ \reset@font%
+ \centering%
+ \@setnobreak%
+ \@setminipage%
+}
+
+
+\long\def\@makefigurecaption#1#2{\footnotesize%
+ \vskip\abovecaptionskip
+\setbox\@tempboxa\hbox{\textbf{#1}\enspace #2}%
+ \ifdim \wd\@tempboxa >\hsize
+ \unhbox\@tempboxa\par
+ \else
+ \hbox to\hsize{\hfil\box\@tempboxa\hfil}%
+ \fi}
+%
+% TABLE
+\newcounter{table}
+\if@secfloat
+ \@addtoreset{table}{section}
+\renewcommand \thetable{\thesection.\@arabic\c@table}
+\else
+ \renewcommand \thetable{\@arabic\c@table}
+\fi
+\def\fps@table{tbp}
+\def\ftype@table{2}
+\def\ext@table{lot}
+\def\fnum@table{\tablename~\thetable.}
+%
+\newenvironment{table}
+ {\let\@makecaption\@maketablecaption%
+ \let\@floatboxreset\@tableboxreset\@float{table}}
+ {\end@float}
+\newenvironment{table*}
+ {\let\@makecaption\@maketablecaption%
+ \let\@floatboxreset\@tableboxreset\@dblfloat{table}}
+ {\end@dblfloat}
+%
+\def\@tableboxreset{%
+ \reset@font%
+ \centering\footnotesize%
+ \def\arraystretch{1.2}
+ \@setnobreak%
+ \@setminipage%
+}
+
+\newlength\abovecaptionskip
+\newlength\belowcaptionskip
+\setlength\abovecaptionskip{8\p@}
+\setlength\belowcaptionskip{3\p@}
+%
+\newdimen\tablewidth \tablewidth\textwidth
+\newdimen\saved@tablewidth \saved@tablewidth\textwidth
+%
+\long\def\@maketablecaption#1#2{%
+ \begingroup%
+ \footnotesize%
+ \global\setbox\@tempboxa\hbox{\textbf{#1}\enspace #2}%
+ \endgroup%
+ \centering%
+ \ifdim \wd\@tempboxa>\tablewidth %
+ \parbox[t]{\tablewidth}{\footnotesize\textbf{#1}\enspace #2\vphantom{Ay}\par}%
+ \else
+ \hbox to\hsize{\hfill\box\@tempboxa\vphantom{Ay}\hfill}%
+ \fi%
+ \global\saved@tablewidth\tablewidth%
+ \global\tablewidth\hsize\vskip\belowcaptionskip}
+%
+%
+%%****************** Algorithm
+\newcounter{algorithm}
+\if@secfloat
+ \@addtoreset{algorithm}{section}
+\renewcommand \thealgorithm{\thesection.\@arabic\c@algorithm}
+\else
+ \renewcommand \thealgorithm{\@arabic\c@algorithm}
+\fi
+\def\fps@algorithm{tbp}
+\def\ftype@algorithm{4}
+\def\ext@algorithm{loa}
+\def\fnum@algorithm{\algorithmname~\thealgorithm.}
+%
+\newenvironment{algorithm}
+ {\let\@makecaption\@makealgorithmcaption%
+ \let\@floatboxreset\@algorithmboxreset\@float{algorithm}}
+ {\end@float}
+\newenvironment{algorithm*}
+ {\let\@makecaption\@makealgorithmcaption%
+ \let\@floatboxreset\@algorithmboxreset\@dblfloat{algorithm}}
+ {\end@dblfloat}
+
+\def\@algorithmboxreset{%
+ \reset@font%
+ \centering
+ \@setnobreak%
+ \@setminipage%
+}
+\long\def\@makealgorithmcaption#1#2{\vskip 2ex \small
+ \hbox to \hsize{\parbox[t]{\hsize}{{\bf #1} #2}}}
+%
+%%%% Program Code:
+\def\programcode{%
+\let\@makealgorithmcaption\@makefigurecaption
+\def\algorithmname{Program Code}}
+
+
+%********************* COMPATIBILITY WITH OLD LATEX:
+\DeclareOldFontCommand{\rm}{\normalfont\rmfamily}{\mathrm}
+\DeclareOldFontCommand{\sf}{\normalfont\sffamily}{\mathsf}
+\DeclareOldFontCommand{\tt}{\normalfont\ttfamily}{\mathtt}
+\DeclareOldFontCommand{\bf}{\normalfont\bfseries}{\mathbf}
+\DeclareOldFontCommand{\it}{\normalfont\itshape}{\mathit}
+\let\sl\it
+\DeclareOldFontCommand{\sc}{\normalfont\scshape}{\@nomath\sc}
+\DeclareRobustCommand*\cal{\@fontswitch\relax\mathcal}
+\DeclareRobustCommand*\mit{\@fontswitch\relax\mathnormal}
+%
+% *********** MATH
+%
+\if@secthm
+ \@addtoreset{thm}{section}
+ \def\thethm{\thesection.\arabic{thm}}
+\else
+ \def\thethm{\arabic{thm}}
+\fi
+%
+%***************************** BIBLIOGRAPHY
+
+\newenvironment{thebibliography}[1]
+ {\section*{\refname}\footnotesize\rmfamily\upshape%
+ \list{\@biblabel{\@arabic\c@enumiv}}%
+ {\settowidth\labelwidth{\@biblabel{#1}}%
+ \leftmargin\labelwidth
+ \setlength\labelsep{8\p@}
+ \advance\leftmargin\labelsep
+ \usecounter{enumiv}%
+ \let\p@enumiv\@empty
+ \renewcommand\theenumiv{\@arabic\c@enumiv}}%
+ \sloppy
+ \clubpenalty4000
+ \@clubpenalty \clubpenalty
+ \widowpenalty4000%
+ \sfcode`\.\@m}
+ {\def\@noitemerr
+ {\@latex@warning{Empty `thebibliography' environment}}%
+ \endlist}
+%
+\newcommand\newblock{\hskip .11em\@plus.33em\@minus.07em}
+%
+\def\@citex[#1]#2{%
+ \let\@citea\@empty
+ \@cite{\@for\@citeb:=#2\do
+ {\@citea\def\@citea{,\penalty\@m\hskip.1pt}%
+ \edef\@citeb{\expandafter\@firstofone\@citeb}%
+ \if@filesw\immediate\write\@auxout{\string\citation{\@citeb}}\fi
+ \@ifundefined{b@\@citeb}{\mbox{\reset@font\bfseries ?}%
+ \G@refundefinedtrue
+ \@latex@warning
+ {Citation `\@citeb' on page \thepage \space undefined}}%
+ {\hbox{\csname b@\@citeb\endcsname}}}}{#1}}
+
+%****************************** FRONTMATTER *
+%
+\newtoks\t@glob@notes
+\newtoks\t@loc@notes
+\newcount\note@cnt
+\newcounter{author}
+\newcount\n@author
+\def\n@author@{}
+\newcounter{address}
+%
+\newcount\sv@hyphenpenalty
+%
+\newcount\prev@elem \prev@elem=0
+\newcount\cur@elem \cur@elem=0
+\chardef\e@pretitle=1
+\chardef\e@title=1
+\chardef\e@subtitle=1
+\chardef\e@author=2
+\chardef\e@address=3
+%
+\newif\if@newelem
+\newif\if@firstauthor
+\newif\if@preface
+\newif\if@hasabstract
+\newif\if@haskeywords
+%
+\newbox\fm@box
+\newdimen\fm@size
+\newbox\t@abstract
+\newbox\t@keywords
+%
+\def\add@tok#1#2{\global#1\expandafter{\the#1#2}}
+\def\add@xtok#1#2{\begingroup
+ \no@harm
+ \xdef\@act{\global\noexpand#1{\the#1#2}}\@act
+\endgroup}
+%
+\def\tailthanksref[#1]#2{\noexpand\pthanksref{#1}}
+\def\pthanksref#1{\global\advance\note@cnt\@ne\ifnum\note@cnt>\@ne
+\global\t@loc@notes\expandafter{\the\t@loc@notes\note@sep}\fi
+\global\t@loc@notes\expandafter{\the\t@loc@notes#1}}
+%
+\def\beg@elem{\global\t@loc@notes={}\global\note@cnt\z@}
+\def\@xnamedef#1{\expandafter\xdef\csname #1\endcsname}
+\def\no@harm{%
+ \let\\=\relax \let\rm\relax
+ \let\ss=\relax \let\ae=\relax \let\oe=\relax
+ \let\AE=\relax \let\OE=\relax
+ \let\o=\relax \let\O=\relax
+ \let\i=\relax \let\j=\relax
+ \let\aa=\relax \let\AA=\relax
+ \let\l=\relax \let\L=\relax
+ \let\d=\relax \let\b=\relax \let\c=\relax
+ \let\bar=\relax
+ \def\protect{\noexpand\protect\noexpand}}
+%
+\def\proc@elem#1#2{\begingroup
+ \no@harm
+ \def\thanks##1##{\@gobble}%
+ \def\thanksref##1##{\@gobble}%
+ \@xnamedef{@#1}{#2}%
+ \endgroup
+ \prev@elem=\cur@elem
+ \cur@elem=\csname e@#1\endcsname
+ \expandafter\elem@nothanksref#2\thanksref\relax%
+ \expandafter\elem@nothanks#2\thanks\relax}
+%
+\def\elem@nothanksref#1\thanksref{\futurelet\@peektok\elem@thanksref}
+\def\elem@thanksref{\ifx\@peektok\relax
+ \else \expandafter\elem@morethanksref \fi}
+\def\elem@morethanksref[#1]#2{\add@thanks{#1}\elem@nothanksref}
+%
+\def\elem@nothanks#1\thanks{\futurelet\@peektok\elem@thanks}
+\def\elem@thanks{\ifx\@peektok\relax
+ \else \ifx\@peektok[ \expandafter\expandafter\expandafter\elem@morethankse
+ \else \expandafter\expandafter\expandafter\elem@morethanks \fi\fi}
+%
+\def\elem@morethankse[#1]#2{\thanks@optarg[#1]{#2}\add@thanks{#1}\elem@nothanks}
+\def\elem@morethanks#1{\thanks@optarg[]{#1}\add@thanks{}\elem@nothanks}
+%
+\def\add@thanks#1{%
+ \global\advance\note@cnt\@ne
+ \ifnum\note@cnt>\@ne \add@xtok\t@loc@notes{\note@sep}\fi
+ \ifx.#1.\add@xtok\t@loc@notes{\thefootnote}\else
+ \add@xtok\t@loc@notes{#1}\fi%
+}
+\def\add@addressref#1{%
+ \global\advance\note@cnt\@ne
+ \ifnum\note@cnt>\@ne \add@xtok\t@loc@notes{\note@sep}\fi
+ \add@tok\t@loc@notes{\ref{#1}}%
+}
+\def\note@sep{,}
+%
+\def\thanks@optarg[#1]#2{%
+ \ifx.#1.\add@tok\t@glob@notes{\footnotetext}%
+ \else\add@tok\t@glob@notes{\freefootnotetext}\fi%
+ \refstepcounter{footnote}%
+ \ifx.#1.\add@xtok\t@glob@notes{[\the\c@footnote]}%
+ \else\add@xtok\t@glob@notes{[#1]}\fi%
+ \add@tok\t@glob@notes{{#2}}%
+ \ignorespaces}%
+%
+% FRONTMATTER
+%
+\def\artty#1{}
+%
+\newdimen\a@title@skip \a@title@skip=12\p@
+\newskip\b@section@skip \b@section@skip=12\p@ plus6\p@ minus6\p@%
+\newskip\b@pretitle@skip \b@pretitle@skip=6\p@
+%
+\def\frontmatter{%
+ \let\@corresp@note\relax
+ \global\t@glob@notes={}\global\c@author\z@
+ \global\c@address\z@
+ \global\n@author=0\n@author@\relax
+ \global\advance\n@author\m@ne
+ \global\@firstauthortrue
+ \global\@hasabstractfalse
+ \global\@prefacefalse
+ \parindent\z@
+ \open@fm \ignorespaces}
+%
+\def\preface{\@prefacetrue}
+%
+% ENDFRONTMATTER
+%
+\def\endfrontmatter{%
+ \global\n@author=\c@author \@writecount
+ \global\@topnum\z@
+ \ifx\@firstpage\@lastpage
+ \gdef\@pagerange{\@firstpage}
+ \else
+ \gdef\@pagerange{\@firstpage--\@lastpage}
+ \fi
+% \thispagestyle{copyright}%
+ \if@twocolumn\else\output@glob@notes\fi
+ \if@preface
+ \@hasabstractfalse
+ \fi
+ \if@hasabstract
+ \normal@text
+ \vskip 18\p@
+ \centering
+ \leavevmode\box\t@abstract\par
+ \fi
+ \if@haskeywords
+ \normal@text
+ \if@hasabstract \vskip6pt\else\vskip18pt\fi
+ \centering
+ \leavevmode\box\t@keywords\par
+ \fi
+ \close@fm
+ \if@twocolumn\output@glob@notes\fi
+ \markboth{\@runauthor\@runtitle}{\@runauthor\@runtitle}%
+ \global\@prefacefalse
+ \global\leftskip\z@
+ \global\@rightskip\z@
+ \global\rightskip\@rightskip
+% \global\c@footnote=0
+ \let\title\relax \let\author\relax
+ \let\address\relax
+ \let\frontmatter\relax \let\endfrontmatter\relax
+ \let\@maketitle\relax \let\@@maketitle\relax
+ \normal@text}
+%
+% Dvieju koloneliu zurnale per visa lapo ploti eina
+% tik pretitle, title ir subtitle. Tam ivedame komanda
+% \maketitle, kuri uzdaro box'a
+
+ \def\two@c@maketitle{%
+ \global\let\close@fm\relax%
+ \vskip\b@section@skip%
+ \par \egroup
+ \emergencystretch=1pc \twocolumn[\unvbox\fm@box]}
+%
+\if@restonecol
+ \let\maketitle\relax
+\else
+ \let\maketitle\two@c@maketitle
+\fi
+%
+
+%
+\newdimen\t@xtheight
+\def\init@settings{
+\splittopskip=\topskip \splitmaxdepth=\maxdepth
+\t@xtheight\textheight \advance\t@xtheight-\splittopskip}
+%
+\def\open@fm{
+ \global\setbox\fm@box=\vbox\bgroup
+ \hsize=\textwidth
+ \centering
+ \sv@hyphenpenalty\hyphenpenalty
+ \hyphenpenalty\@M}
+%
+
+\def\close@fm{%
+ \vskip\b@section@skip%
+ \par \egroup
+ \if@twocolumn\else%
+ \fm@size=\dp\fm@box \advance\fm@size by \ht\fm@box
+ \@whiledim\fm@size>\t@xtheight \do{%
+ \global\setbox\@tempboxa=\vsplit\fm@box to \t@xtheight
+ \unvbox\@tempboxa \newpage
+ \fm@size=\dp\fm@box \advance\fm@size by \ht\fm@box}
+ \fi%
+ \if@twocolumn
+ \emergencystretch=1pc \twocolumn[\unvbox\fm@box]
+ \else
+ \unvbox\fm@box
+ \fi}
+%
+\def\output@glob@notes{\bgroup
+ \the\t@glob@notes
+ \egroup}
+%
+\def\justify@off{\let\\=\@normalcr
+ \leftskip\z@ \@rightskip\@flushglue \rightskip\@rightskip}
+\def\justify@on{\let\\=\@normalcr
+ \parfillskip\@flushglue%
+ \leftskip\z@ \@rightskip\z@ \rightskip\@rightskip}
+%
+\def\normal@text{\global\let\\=\@normalcr
+ \global\leftskip\z@ \global\@rightskip\z@ \global\rightskip\@rightskip
+ \global\parfillskip\@flushglue}
+%
+\def\@writecount{\write\@mainaux{\string\global
+ \string\@namedef{n@author@}{\the\n@author}}%
+}
+%
+% TITLE
+\def\pretitle#1{%
+\vspace*{\b@pretitle@skip}\pretitle@size#1\par\vskip6\p@\hrule
+\vskip12\p@}
+%
+\def\title#1{%
+ \beg@elem
+ \title@note@fmt
+ \add@tok\t@glob@notes
+ {\title@note@fmt}%
+ \proc@elem{title}{#1}%
+ \def\title@notes{\the\t@loc@notes}%
+ \title@fmt{\@title}{\title@notes}%
+ \ignorespaces}
+%
+\newdimen\@@topskip \@@topskip=24\p@
+%
+\def\title@fmt#1#2{%
+ \vspace*{\@@topskip}
+ {\title@size #1\hbox{$^{#2}$}\par}%
+ \vskip\a@title@skip%
+ }
+
+%
+\def\subtitle#1{%
+ \beg@elem
+ \proc@elem{subtitle}{#1}%
+ \def\title@notes{\the\t@loc@notes}%
+ \subtitle@fmt{\@subtitle}{\title@notes}%
+ \ignorespaces}
+%
+%
+\def\subtitle@fmt#1#2{%
+ {\subtitle@size #1\,\hbox{$^{\mathrm{#2}}$}\par}%
+ \vskip\a@title@skip%
+ }
+%
+\def\title@note@fmt{\def\thefootnote{\arabic{footnote}}}
+%
+% AUTHOR
+%
+\newdimen\b@author@skip
+\b@author@skip 12\p@
+%
+\def\author{\@ifnextchar[{\author@optarg}{\author@optarg[]}}
+%
+\def\author@optarg[#1]#2{\stepcounter{author}%
+ \beg@elem\def\degs##1{##1}\def\fnms##1{##1}\def\inits##1{##1}%
+ \def\snm##1{\MakeUppercase{##1}}\def\roles##1{##1}%
+ \if@firstauthor%
+ \first@author \global\@firstauthorfalse \fi%
+ \@for\@tempa:=#1\do{\expandafter\add@addressref\expandafter{\@tempa}}%
+ \proc@elem{author}{#2}%
+ \author@fmt{\the\c@author}{\the\t@loc@notes}{\@author}}%
+%
+%\newbox\author@box
+
+%
+\def\author@fmt#1#2#3{\@newelemtrue
+ \ifnum\prev@elem=\e@author \global\@newelemfalse \fi
+ \if@newelem \author@fmt@init \fi
+ \edef\@tempb{#2}\ifx\@tempb\@empty
+ \hbox{#3}\else
+ \hbox{#3\,$^{\mathrm{#2}}$}%
+ \fi}
+%
+\def\first@author{\author@note@fmt%
+ \add@tok\t@glob@notes%
+ {\author@note@fmt}}%
+%
+\def\author@fmt@init{%
+ \par
+ \vskip \b@author@skip
+ \authors@size\centering
+ \leavevmode}
+%
+\def\and{\unskip~and~}
+%
+\def\author@note@fmt{%
+ \def\thefootnote{\arabic{footnote}}}
+%
+\def\sxarabic#1{%
+ \expandafter\ifcase\value{#1} \or *\or **\or *** \or **** \or *****\fi
+}
+%
+% ADDRESS
+%
+\def\email#1{{e-mail:\ #1}}
+%
+\def\address{\@ifstar{\address@star}%
+ {\@ifnextchar[{\address@optarg}{\address@noptarg}}}
+%
+\def\address@optarg[#1]#2{\refstepcounter{address}%
+ \beg@elem
+ \proc@elem{address}{#2}%
+ \address@fmt{\the\c@address}{\the\t@loc@notes}{\@address}\label{#1}%
+ \ignorespaces}
+%
+\def\address@noptarg#1{\refstepcounter{address}%
+ \beg@elem
+ \proc@elem{address}{#1}%
+ \address@fmt{\z@}{\the\t@loc@notes}{\@address}%
+ \ignorespaces}
+%
+\def\address@star#1{%
+ \beg@elem
+ \proc@elem{address}{#1}%
+ \address@fmt{\m@ne}{\the\t@loc@notes}{\@address}%
+ \ignorespaces}
+%
+\def\theaddress{\alph{address}}
+%
+\def\address@fmt#1#2#3{\@newelemtrue
+ \ifnum\prev@elem=\e@address \@newelemfalse \fi
+ \if@newelem \address@fmt@init \fi
+ \bgroup\parskip\z@\noindent\centering \address@size
+ \ifnum#1=\z@
+ #3\,$^{\mathrm{#2}}$\space%
+ \else
+ \ifnum#1=\m@ne
+ $^{\phantom{\mathrm{\theaddress}}\,}$#3\,$^{\mathrm{#2}}$%
+ \else
+ $^{\mathrm{\theaddress}\,}$#3\,$^{\mathrm{#2}}$%
+ \fi
+ \fi
+ \par\egroup}
+%
+\def\address@fmt@init{%
+ \def\@currentlabel{\theaddress}
+ \par
+ \vskip 2\p@ plus 1\p@ minus 1\p@}
+%
+% ABSTRACT
+%
+\def\abstract{\@ifnextchar[{\@abstract}{\@abstract[]}}
+\def\@abstract[#1]{%
+ \global\@hasabstracttrue
+ \hyphenpenalty\sv@hyphenpenalty
+ \global\setbox\t@abstract=\vbox\bgroup
+ \linewidth\abstract@width
+ \hsize\abstract@width
+ \justify@on\abstract@size\parindent 1em
+ \abstract@indent\textbf{\abstractname}\ignorespaces}
+\def\endabstract{\par\egroup}
+%
+% KEYWORDS
+\def\sep{\unskip, }
+\global\@haskeywordsfalse
+\newdimen\dp@t@keywords
+\def\keyword{\global\@haskeywordstrue%
+ \global\setbox\t@keywords=\vbox\bgroup%
+ \hsize\abstract@width%
+ \justify@on\abstract@size\parindent 0\p@
+ \textbf{\keywordsname}\ignorespaces
+ }
+\def\endkeyword{\par\egroup\global\dp@t@keywords=\dp\t@keywords}
+\def\keywords#1{\begin{keyword}#1\end{keyword}}
+%
+%
+%
+% Running title
+\def\runningtitle#1{\gdef\@runtitle{#1}} \def\@runtitle{}
+\def\runningauthor#1{{\def\etal{et al.}\gdef\@runauthor{#1\@runsep}}} \def\@runauthor{}
+\def\runningsep#1{\gdef\@runsep{#1}}
+\def\@runsep{\ /\ }
+%
+\def\journal#1{\gdef\@journal{#1}} \@ifundefined{@journal}{\gdef\@journal{Journal not defined}}{}
+\def\volume#1{\gdef\@volume{#1}} \def\@volume{0}
+\def\issue#1{\gdef\@issue{#1}} \def\@issue{0}
+%
+%
+\newcount\@pubyear
+\newcount\@copyear
+\@pubyear=\number\year
+\@copyear\@pubyear
+\advance\@copyear-2000
+
+\def\pubyear#1{\global\@pubyear#1
+ \global\@copyear\@pubyear
+ \global\advance\@copyear-2000%
+ \ignorespaces}
+%
+\def\the@copyear{\ifnum\@copyear<10 0\fi\the\@copyear}
+
+%
+\pubyear{2003}
+%
+\def\firstpage#1{\def\@tempa{#1}\ifx\@tempa\@empty\else
+ \gdef\@firstpage{#1}\gdef\@lastpage{#1}%
+ \global\c@page=#1 \ignorespaces\fi
+ }
+\def\@firstpage{1}
+\def\lastpage#1{\def\@tempa{#1}\ifx\@tempa\@empty\else
+ \gdef\@lastpage{#1}\ignorespaces\fi}
+\def\@lastpage{0}
+\def\@pagerange{1--0}
+
+% Write the last page:
+\def\write@last@page{%
+\write\@mainaux{\string\global\string\@namedef{@lastpage}{\the\c@page}}}
+
+\AtEndDocument{\write@last@page}
+% SGML
+\long\def\convertas#1#2{#2}
+\def\sday#1{#1}\def\smonth#1{#1}\def\syear#1{#1}
+\def\aid#1{\gdef\@aid{#1}}
+%
+\def\SSDI#1{\gdef\@ssdi{#1}} \def\@ssdi{000000-00}
+\def\issn#1{\gdef\@issn{#1}}
+\def\price#1{\gdef\@price{#1}}
+%
+\def\date#1{\gdef\@date{#1}} \def\@date{\today}
+%
+
+\def\empty@data{\@nil}
+%
+
+%***************** BACKMATTER
+\newcommand\backmatter{\goodbreak}
+
+%**************** INICIALIZATION
+\newcommand\refname{References}
+\newcommand\figurename{Figure}
+\newcommand\tablename{Table}
+\newcommand\algorithmname{Algorithm}
+\newcommand\appendixname{Appendix}
+\newcommand\abstractname{Abstract. }
+\newcommand\keywordsname{Keywords. }
+\def\acknowledgementsname{Acknowledgements}
+%
+\def\copyright@sign{\copyright}
+%
+% DIMENSIONS
+\def\@articletypesize{\large}
+\def\pretitle@size{\LARGE}
+\def\title@size{\huge}
+\def\subtitle@size{\large\itshape}
+\def\authors@size{\normalsize}
+\def\abstract@size{\footnotesize}
+\def\abstract@width{22pc}
+\def\abstract@indent{\noindent}
+\def\address@size{\normalsize\itshape}
+% Block preparation of contents:
+\def\addcontentsline#1#2#3{}
+\long\def\addtocontents#1#2{}
+%
+\newcommand\today{}
+\edef\today{\ifcase\month\or
+ January\or February\or March\or April\or May\or June\or
+ July\or August\or September\or October\or November\or December\fi
+ \space\number\day, \number\year}
+%
+\@twosidetrue
+\pagenumbering{arabic}
+\frenchspacing
+\init@settings
+
+\if@twocolumn\setlength\tablewidth{\columnwidth}
+\else\setlength\tablewidth{\textwidth}\fi
+%\pagestyle{headings}
+\pagestyle{empty}
+
+\endinput
+%%
+%% End of file `IOS-Book-Article.cls'.
diff --git a/theory/Papers/Parco_2017/main.tex b/theory/Papers/Parco_2017/main.tex
new file mode 100644
index 0000000000000000000000000000000000000000..2eccddafeb61eb3c06e3d612492434dff1e3272b
--- /dev/null
+++ b/theory/Papers/Parco_2017/main.tex
@@ -0,0 +1,385 @@
+\documentclass{IOS-Book-Article}
+
+\usepackage{mathtools, mathptmx, amsmath, amsthm, amssymb}
+\usepackage{graphicx, subcaption}
+\usepackage{listings}
+\usepackage{caption}
+\usepackage{multirow}
+\usepackage{color}
+\usepackage{cite, hyperref}
+\usepackage{siunitx}
+\usepackage{xspace}
+\usepackage{makecell}
+
+\renewcommand\theadalign{cb}
+\renewcommand\theadfont{\bfseries}
+\renewcommand\theadgape{\Gape[4pt]}
+\renewcommand\cellgape{\Gape[4pt]}
+\renewcommand{\ttdefault}{pcr}
+
+\renewcommand{\thesubfigure}{\arabic{subfigure}}
+
+% Some colors
+\definecolor{gray}{gray}{0.3}
+\definecolor{graybox}{gray}{0.8}
+
+% Some acronyms
+\newcommand{\swift}{{\sc Swift}\xspace}
+\newcommand{\gadget}{{\sc Gadget-2}\xspace}
+\newcommand*\mymin[1][]{\min_{#1}\,}
+
+\renewcommand{\lstlistingname}{\textbf{Code}}% Listing -> Code
+\captionsetup[lstlisting]{singlelinecheck=false, margin=0pt,labelfont=bf,font=scriptsize}
+
+\def\hb{\hbox to 10.7 cm{}}
+
+\begin{document}
+
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+% Set options for the listings package %
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+\lstset{%
+ language=c,
+ basicstyle=\scriptsize\ttfamily,
+ keywordstyle=\bfseries,
+ commentstyle=\color{gray},
+ rulecolor=\color{black},
+ framerule=0.6pt,
+ numbers=left,
+ numberstyle=\tiny,
+ escapeinside={@}{@},
+ captionpos=b
+ }
+
+\pagestyle{headings}
+\def\thepage{}
+
+\begin{frontmatter} % The preamble begins here.
+
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+% Title, author and affiliations %
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+\title{An Efficient SIMD Implementation of Pseudo-Verlet Lists for Neighbour Interactions in Particle-Based Codes}
+
+\markboth{}{September 2017\hb}
+
+\author[A]{\fnms{James S.} \snm{Willis}%
+\thanks{Corresponding Author; E-mail:\url{james.s.willis@durham.ac.uk.}}},
+\author[A]{\fnms{Matthieu} \snm{Schaller}},
+\author[B,C]{\fnms{Pedro} \snm{Gonnet}}
+\author[A]{\fnms{Richard G.} \snm{Bower}}
+and
+\author[A]{\fnms{Peter W.} \snm{Draper}},
+
+\runningauthor{Institute for Computational
+Cosmology (ICC),
+Department of Physics,
+Durham University,
+Durham DH1 3LE, UK}
+\address[A]{Institute for Computational
+Cosmology (ICC),
+Department of Physics,
+Durham University,
+Durham DH1 3LE, UK}
+\address[B]{School of Engineering and
+Computing Sciences,
+Durham University,
+Durham DH1 3LE, UK}
+\address[C]{Google Switzerland GmbH,
+8002 Z{\"u}rich, Switzerland}
+
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+% Abstract %
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+\begin{abstract}
+In particle-based simulations, neighbour finding (i.e finding pairs of particles to interact within a given range) is the most time consuming part of the computation. One of the best such algorithms, which can be used for both Molecular Dynamics (MD) and Smoothed Particle Hydrodynamics (SPH) simulations, is the pseudo-Verlet list algorithm. This algorithm, however, does not vectorize trivially, and hence makes it difficult to exploit SIMD-parallel architectures. In this paper, we present several novel modifications as well as a vectorization strategy for the algorithm which lead to overall speed-ups over the scalar version of the algorithm of 2.24x for the AVX instruction set (SIMD width of 8), 2.43x for AVX2, and 4.07x for AVX-512 (SIMD width of 16).
+\end{abstract}
+
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+% Metadata %
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+\begin{keyword}
+Particle Methods; Smoothed Particle Hydrodynamics; Molecular Dynamics; SIMD; Applications
+\end{keyword}
+\end{frontmatter}
+\markboth{J.~Willis, M.~Schaller, P.~Gonnet, R. Bower~\&~P.~Draper 2017 \hb}{SIMD pseudo-Verlet list for particle-based codes\hb}
+
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+% Introduction %
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+\section{Introduction}
+\label{ref:introduction}
+
+Particle-based simulations are widely used in many research fields, e.g. chemistry, physics, biology. The under-lying algorithm evolves a system of particles via a set of pairwise interactions. Short-range interactions are evaluated by computing pairwise distances between particles and checking that they lie within a cut-off radius, $h$, of each other (see Figure~\ref{fig:sph}).
+
+Computing the short-range pairwise distances between particles takes up a large fraction of the CPU time for these simulations. For $N$ particles, a naive implementation involves $\mathcal{O}(N^2)$ operations, which can be expensive to compute. The number of distance calculations can be significantly reduced by using a cell list \cite{ref:Cell_list}, that decomposes the domain into cells of edge length $C_l \geqslant h$ such that each particle can find its neighbours by searching only in the local or neighbouring cells.
+
+However, cell lists are still far from optimal, as it can be shown that for a uniform distribution of particles in two neighbouring cells (sharing a face) only $\leqslant$16\% of particle pairs will meet the criteria $r^2 \leqslant h^2$, where $r$ is the separation between particles \cite{ref:PG_cell_orientations}. This leads to $\geqslant$84\% unnecessary distance calculations between pairs of cells (see Figure~\ref{fig:sph} for a 2D example). This fraction can be reduced using the pseudo-Verlet list algorithm\cite{ref:PG_Pseudo_Verlet_list}. But the pseudo-Verlet list algorithm, due to its branching and inherently inefficient memory access patterns, does not lend itself to automatic SIMD-vectorization, which is crucial for obtaining the best possible performance on modern CPU architectures. We therefore, in this paper, present a SIMD vectorization strategy for the pseudo-Verlet list that addresses these issues.
+
+This optimisation strategy can be applied to Molecular Dynamics (MD) and Smoothed Particle Hydrodynamics (SPH) codes widely used in chemistry and physics. We have chosen to implement our SIMD strategy in \swift\footnote{\url{www.swiftsim.com}}, a cosmological simulation code \cite{ref:SWIFT_SIAM, ref:SWIFT_PASC} that solves the equations of hydrodynamics using SPH (See \cite{ref:SPH_review} for a review).
+
+\begin{figure}
+ \centering
+ \includegraphics[width=0.6\textwidth]{Figures/sph.eps}
+ \caption{Computing the interactions of a set of $N$ particles using Smoothed Particle Hydrodynamics. Each particle finds its neighbours by computing $N - 1$ pairwise distances and checking whether they fall within a cut-off radius, $h_i$. The particle's density is then found by computing a weighted sum over all its neighbours, where the weight decreases with distance from the particle up to $h_i$.}
+ \label{fig:sph}
+\end{figure}
+
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+% Method %
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+\section{Pseudo-Verlet Lists} \label{sec:pVl}
+
+For the cell-based neighbour search, the simulation domain is first decomposed into cells of edge length $C_l \geqslant h$, and the particles corresponding to each cell are stored together. When searching for neighbours spanning a pair of cells, it is sufficient to loop over the particles of both cells and check if all possible particle pairs are within range of each other, e.g.
+
+\begin{lstlisting}[caption={Simple iteration over neighbours.}, label=code:naive_pair]
+for (int i = 0; i < count_a; i++)
+ for (int j = 0; j < count_b; j++)
+ r = particle_dist(parts_a[i], parts_b[j]);
+ if (r < h)
+ // Compute interaction.
+\end{lstlisting}
+
+\noindent where {\tt parts\_a} and {\tt parts\_b} are the particles in the neighbouring cells, and {\tt count\_a} and {\tt count\_b} their respective counts. Although much more efficient than the naive $\mathcal{O}(N^2)$ algorithm, less than $16\%$ of the particle pairs inspected will actually be within $h$ of each other (see Figure~\ref{fig:sph}), resulting in a large number of spurious pairwise distance calculations.
+
+The pseudo-Verlet list algorithm \cite{ref:PG_Pseudo_Verlet_list} improves on the cell list algorithm by first projecting the particle positions from both cells onto the axis joining the cell centers. The particles in each cell are then sorted with respect to their position along this axis, resulting in the arrays {\tt dist} and {\tt index} containing the distance on the axis and its corresponding particle respectively. Given these two arrays for each cell, we can find the neighbours as follows
+
+\begin{lstlisting}[caption={Pseudo-Verlet list iteration over neighbours.}, label=code:scalar_verlet_list]
+for (int i = 0; i < count_a; i++)
+ for (int j = 0; j < count_b @\colorbox{graybox}{\&\& dist\_b[j] < dist\_a[i] + h}@; j++)
+ r = particle_dist(parts_a[index_a[i]], parts_b[index_b[j]]);
+ if (r < h)
+ // Compute interaction.
+\end{lstlisting}
+
+The {\tt dist} and {\tt index} arrays need to be pre-computed for every configuration of neighbouring cells, e.g. cell pairs sharing a common face, a common edge, or a common corner, which reduces to 13 distinct directions if symmetries are exploited. If in the inner loop we replace {\tt dist\_a[i] + h} with {\tt dist\_a[i] + h + max\_dx}, where {\tt max\_dx} is the maximum displacement of any particle in cell $a$, then we can re-use the sorted indices over several time steps, as is described in \cite{ref:PG_Pseudo_Verlet_list}.
+
+Using this scheme, about 68\% of particle pairs inspected will be within range of each other, which is a significant improvement over the 16\% in the naive algorithm. The increased performance, however, comes at a cost in complexity: whereas the naive algorithm vectorizes trivially, the pseudo-Verlet algorithm, with its additional loop exit condition and out-of-order access to the particle data, does not.
+
+\begin{figure}
+ \centering
+ \begin{subfigure}[b]{0.55\textwidth}
+ \includegraphics[width=1\linewidth]{Figures/parts_sorted.eps}
+ \end{subfigure}
+
+ \begin{subfigure}[b]{0.55\textwidth}
+ \includegraphics[width=1\linewidth]{Figures/parts_on_axis.eps}
+ \end{subfigure}
+
+ \caption{Performing cell-pair interactions using a sorted pseudo-Verlet list. \textit{Top:} Particles are projected onto the cell-pair axis and sorted according to their distance along the axis. The particles $p_i^{(a)}$ on the left (cell ($a$)) receive contributions from the particles $p_j^{(b)}$ on the right (cell ($b$)). \textit{Bottom:} Each particle is traversed and a pairwise distance calculation is only performed for particles in ($b$) that are within $h_i$ on the axis as this provides an upper-bound on the 3D distance. Interactions are later computed for the particles $p_i^{(a)}$ that obey $ \|p^{(a)}_i - p^{(b)}_j\|_2 < h_i^{(a)}$.}
+ \label{fig:sort_parts}
+\end{figure}
+
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+% Implementation %
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+\section{SIMD Implementation}
+\label{sec:simd_implementation}
+
+The optimisations are split between the neighbour search part of the algorithm, which can be applied to any particle-based code, and the particle interaction function.
+
+Most compilers (Intel, GNU and Clang) fail to auto-vectorise the algorithm efficiently due to multiple exit conditions and conditional statements (see lines 2 and 4 of Code \ref{code:scalar_verlet_list}). We therefore decided to perform explicit vectorization of the code using vector intrinsics\cite{ref:intel_intrinsics_guide}, which allows us to achieve the same level of performance across different compilers. In the following we outline a series of modifications that improve the performance of the code.
+
+\subsection{General SIMD Strategy}
+
+The overall vectorization strategy involved picking one particle, $p^{(a)}_i$, from the left-hand cell ($a$) and interacting it with a vector length of, $p^{(b)}_j$, particles that are within range from the right-hand cell ($b$). The particles, $p^{(a)}_i$, are traversed in reverse along the axis, i.e. starting from the cell interface and moving away from it. A pairwise distance calculation is only performed with particles, $p^{(b)}_j$ that lie within $h^{(a)}_i$, the cut-off radius of $p^{(a)}_i$, on the sorted axis. If any particles $p^{(b)}_j$ satisfy the criterion $\|p^{(a)}_i - p^{(b)}_j\|_2 < h^{(a)}_i$, where $\|\cdot\|_2$ denotes the Euclidean distance between two particles, an interaction is computed. The contributions from the $p^{(b)}_j$ that are not within range are masked out. This method is illustrated on Figure~\ref{fig:sort_parts}.
+
+As the particle interaction functions are straight-forward, their vectorization is not particularly interesting and we will therefore focus on the neighbour search part of the algorithm in the following.
+
+\subsection{Particle Caching}
+\label{sec:particle_caching}
+
+We create a {\em particle cache} that only contains the subset of particle properties needed for an interaction. The particles are cached in sorted order along the cell-pair axis, using the sorted list of particle indices from the Verlet list. This cache is laid out using a structure of arrays (SoA) data layout and is only performed for sections of the code that include particle interaction. Although creating and filling this cache incurs an additional computational cost, this overhead is amortised with the improved memory access patterns for the SIMD implementation.
+
+A side benefit is that the particle positions can be reduced from double to single precision values in this step. In order to retain numerical precision, we first shift the positions by the center of the cell-pair $c$, wrapping for boundary conditions, and then convert them to single precision, e.g. $x_{\mathtt{single}} = x_{\mathtt{double}} - c$. This allows for a more efficient use of the vector processing units whilst preventing numerical cancellation when computing the pairwise distances.
+
+\subsection{Lowering the Number of Pairwise Distance Calculations}
+\label{sec:max_d}
+
+Computing the pairwise distances between particles (line 3 of Code \ref{code:scalar_verlet_list}) is the most time-consuming part of the neighbour search algorithm. In order to reduce the number of distance calculations, we find the {\em leftmost} particle in cell ($a$) which is in range of any of the particles in cell ($b$), e.g.
+
+\begin{lstlisting}
+int first_a = count_a;
+while (first_a > 0 && dist_a[first_a - 1] + h_max_a > dist_b[0])
+ first_a--;
+\end{lstlisting}
+
+We then introduce the array {\tt max\_index\_a} which contains, for each particle in cell ($a$), the index of the farthest possible interacting particle in cell ($b$). This array is constructed as follows:
+
+\begin{lstlisting}
+int temp = 0;
+while (temp < count_b - 1 &&
+ (dist_a[first_a] + parts_a[index_a[first_a]].h > dist_b[temp])) temp++;
+max_index_a[first_a] = temp;
+for (i = first_a + 1; i < count_a; i++)
+ temp = max_index_a[i - 1];
+ while (temp < count_b - 1 &&
+ (dist_a[i] + parts_a[index_a[i]].h > dist_b[temp])) temp++;
+ max_index_a[i] = temp;
+\end{lstlisting}
+
+\noindent For each {\tt i}th particle in cell ($a$) from {\tt first\_a} to {\tt count\_a}, we only need to inspect the particles in cell ($b$) from {\tt 0} to {\tt max\_index\_a[i]} (see Figure~\ref{fig:read_cache_subset}). By consequence, only the particles from cell ($b$) from {\tt 0} to {\tt max\_index\_a[count\_a - 1]} need to be loaded into the particle cache. Note that we compute {\tt max\_index\_a} as an approximate value using only a single pass over the particles; we could compute an exact value but it would require $\mathcal{O}(N^2)$ operations.
+
+Since we are computing interactions symmetrically, we compute the same indices for particles in cell ($b$) interacting with particles in cell ($a$), i.e. {\tt last\_b} and {\tt min\_index\_b} respectively, and cache the particles accordingly. We therefore have to be careful to cache the union of the set of particles from both cells required for interactions in both directions.
+
+\begin{figure}
+ \centering
+ \includegraphics[width=0.6\textwidth]{Figures/read_cache_subset.eps}
+ \caption{For a given particle $p_i^{(a)}$ (red circles), only the particles within a distance $d_i^{(a)}+h_{\rm max}^{(a)}$ (yellow circles) are candidates for interactions in cell ($b$). These particles are located between index {\tt 0} and {\tt max\_index\_a[i]} in the sorted array of particles of cell ($b$).}
+ \label{fig:read_cache_subset}
+\end{figure}
+
+\subsection{Final Interaction Loop}
+\label{sec:final_loop}
+
+Once we have calculated the loop bounds, we find the particle neighbours and perform the interaction:
+
+\begin{lstlisting}
+for (int i = first_a; i < count_a; i++)
+ for (int j = 0; j <= max_index_a[i]; j += SIMD_LENGTH)
+ simd_r = particle_dist_simd(i, j);
+ mask = (simd_r < SIMD(parts_a[index_a[i]].h));
+ if (ANY(mask))
+ particle_interact_simd(i, j, mask);
+\end{lstlisting}
+
+\noindent where {\tt particle\_dist\_simd(i, j)} returns a SIMD vector containing the pairwise distances between the cached particle data from cell ($a$) at position {\tt i} and the {\tt SIMD\_LENGTH} cached particle positions from cell ($b$) starting at index {\tt j}. Similarly, \texttt{particle\_interact\_simd(i, j, mask)} computes the interactions between the particle at index {\tt i} and the particles as of index {\tt j} using the provided {\tt mask}. Note that in practice, {\tt max\_index\_a[i]} is padded to a multiple of the SIMD width of the instruction set used. The results of the interactions on particle {\tt i} are stored in a SIMD vector and only aggregated horizontally and stored only once at the end of the innermost loop (not shown in code).~\\
+
+
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+% Results %
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+\section{Results}
+
+In this section we present results obtained on different instruction sets using a standardized benchmark of the core compute kernels of the cosmological SPH code \swift\cite{ref:SWIFT_PASC}. The benchmark, named {\em test27cells}, computes the interactions between one cell containing $216$ randomly placed particles and its $26$ neighbours which are similarly populated. This allows us to probe the speed-up from vectorization in all the relevant geometrical configurations, and is representative of the workload in actual production runs using \swift. All results reported here are based on revision \texttt{11518ff7} of \swift, which implements the algorithm described in Section~\ref{sec:simd_implementation}.
+
+Internally, \swift uses a set of macros that map a common set of intrinsics to their equivalents for each specific instruction set. The same user code is used for all cases but the actual underlying compiled code will be architecture-specific. We currently support the AVX, AVX2 and AVX-512 architectures, but the common intrinsics can easily be extended to other instruction sets such as AltiVec or ARM NEON.
+
+\subsection{Platforms, Compiler, and Methodology}
+
+Table~\ref{table:machines_benchmark} lists the main characteristics of the machines used for our benchmarks. On all three systems we used the Intel compiler v.17.0.2 with the \texttt{-O3} flag alongside the respective SIMD-specific flags. We additionally used the \texttt{-no-vec} and \texttt{-no-simd} flags to produce the scalar code used in the comparisons.
+
+\begin{table}[h]
+ \centering
+ \caption{Machines used for benchmarking. The KNL processor was placed in \textit{Flat-Quadrant} mode.}
+ \label{table:machines_benchmark}
+ \begin{tabular}{ clccc }
+ \hline
+ \hline
+ Machine Name & \makecell{Processor} & Cores & Vector ISA & Clock Rate [GHz]\\
+ \hline
+ COSMA-5 & Intel Xeon E5-2670 (Sandy Bridge) & 2 $\times$ 8 & AVX & 2.6 \\
+ Hamilton & Intel Xeon E5-2650 (Broadwell) & 2 $\times$ 12 & AVX2 & 2.2 \\
+ Kyll & Intel Xeon Phi 7210 (Knights Landing) & 1 $\times$ 64 & AVX-512 & 1.3 \\
+ \hline
+ \hline
+ \end{tabular}
+\end{table}
+
+To obtain precise execution times we use the {\tt RDTSC} cycle counter and convert the cycle counts to milliseconds using the clock-speed of each platform. All benchmarks are run using a single thread and we report the median time of 5 independent runs.
+
+\subsection{Idealised Particle Interaction Speed-ups}
+
+We start by reporting the speed-up of the raw particle interactions, i.e. in the absence of any neighbour search. This highly idealised test assumes that all particles are always in range of each other, hence using SIMD vector instructions with full masks. This represents the hypothetical maximal speed-up that can be achieved for this problem and provides an upper-bound on the possible speed-up that can be achieved with the pseudo-Verlet list algorithm. This test interacts one particle with $2560$ other particles by directly calling the interaction function {\tt particle\_interact\_simd(i, j, mask)} with a full {\tt mask}. Table~\ref{table:raw_interaction_results} lists the times of both the scalar and vectorized functions.
+
+\begin{table}[h]
+ \centering
+ \caption{Median times and corresponding vectorization speed-ups for the idealized case of one particle directly interacting with $2560$ other particles without any distance checks.}
+ \label{table:raw_interaction_results}
+ \begin{tabular}{ clccc }
+ \hline
+ \hline
+ \makecell{Machine Name\\~} & \makecell{CFLAGS\\~} & \makecell{Scalar Time [ms] \\ (\texttt{-no-vec -no-simd})} & \makecell{Vectorised Time [ms] \\ ~} & \makecell{Speed-up\\~} \\
+ \hline
+ COSMA-5 & \texttt{-xAVX} & $0.048$ & $0.0084$ & 5.66x \\
+ Hamilton & \texttt{-xCORE-AVX2} & $0.038$ & $0.0055$ & 6.77x \\
+ Kyll & \texttt{-xMIC-AVX512} & $0.170$ & $0.0079$ & 21.30x \\
+ \hline
+ \hline
+ \end{tabular}
+\end{table}
+
+The difference between the AVX and AVX2 results (both using 256-bit long vectors) is due to the use of Fused Multiply-Add {\em FMA} instructions in the AVX2 set. Similarly, the speed-up for the AVX-512 instruction set exceeds the vector length of 16 due to the use of FMAs.
+These results demonstrate that, as expected due to their simple structure (no branching), the interaction functions themselves vectorize extremely well.
+
+The results in Table~\ref{table:raw_interaction_results} compare favourably to those of \cite{ref:Luigi_Gadget} who reported a vectorization speed-up of 6.62x on KNL (AVX-512) and 2.20x on Ivy-Bridge (AVX) when analysing a similar loop over neighbours in their improved version of the \gadget code\cite{ref:Gadget}. The difference might, in part, be explained by their use of double-precision arithmetic throughout.
+
+\subsection{Pseudo-Verlet List SIMD Speed-ups}
+
+As the number of particle pairs probed in the pseudo-Verlet algorithm depend on the orientation of the pair of cells, we break down the results into cell pairs sharing either a {\em corner}, an {\em edge}, or a {\em face}. We then compute a weighted total (i.e. $8\times\mathrm{corner}+12\times\mathrm{edge}+6\times\mathrm{face}$) to obtain the speed-up corresponding to a realistic scenario where all 26 cell-pair orientations have to be computed. Table~\ref{table:cell_orientation_results} lists the results obtained using the AVX instruction set on COSMA-5.
+
+\begin{table}[h]
+ \caption{Median times and corresponding speed-ups of the full SIMD pseudo-Verlet list algorithm implemented using the AVX instruction set on COSMA-5. Results for each geometrical configuration of the cell-pairs are reported as well as for the weighted total.}
+ \label{table:cell_orientation_results}
+ \centering
+ \begin{tabular}{ cccc }
+ \hline
+ \hline
+ \makecell{Cell-pair \\ Orientation} & \makecell{Scalar Time [ms] \\ (\texttt{-no-vec -no-simd})} & \makecell{Vectorised Time [ms] \\ (AVX)} & \makecell{Speed-up\\~} \\
+ \hline
+ Corner & $0.00035$ & $0.00070$ & 0.49x \\
+ Edge & $0.0052$ & $0.0035$ & 1.48x \\
+ Face & $0.082$ & $0.034$ & 2.41x \\
+ \hline
+ {\em Total} & $0.56$ & $0.25$ & 2.21x \\
+ \hline
+ \hline
+ \end{tabular}
+\end{table}
+
+As expected, the results show a strong dependence of both the times and the speed-ups on the cell-pair orientation. Since a corner cell-pair will typically interact only one or two particles, the near-constant cost of populating the cache and computing the loop exit condition cannot be amortized by the higher speed at which the interactions can be processed. However, the total time spent in corner configurations is negligible and does not significantly affect the total speed-up. In \swift we therefore use the scalar code for the corner configurations, which leads to a weighted total speed-up over the 26 cell-pair configurations of 2.24x.
+
+Both the edge and face cases show speed-ups from vectorization and the gain is larger when more particles interact (face vs. edge) as the constant vectorization cost can be more easily amortized. The best speed-up obtained (2.41x) is far from the theoretical maximum for AVX (8x) but compares well to the raw interaction speed-ups (5.66x). The difference in performance arises from the constant cost of populating the cache, and additional complexity of computing distances and masking of out-of-range interactions which leads to partially full masks, especially for the edge-orientation case. Given the complexity of the algorithm we conclude that 2.41x is a good speed-up.
+
+In Table~\ref{table:pseudo_verlet_list_simd_results} we present the median times and speed-ups for the weighted sum of all cell-pair orientations, for the three available instructions sets.
+
+\begin{table}[h]
+ \caption{Median times and corresponding speed-ups of the full SIMD pseudo-Verlet list algorithm for the weighted sum of all cell-pair orientations implemented using the AVX, AVX2 and AVX-512 instruction sets.}
+ \label{table:pseudo_verlet_list_simd_results}
+ \centering
+ \begin{tabular}{ clccc }
+ \hline
+ \hline
+ \makecell{Machine Name\\~} & \makecell{CFLAGS\\~} & \makecell{Scalar Time [ms] \\ (\texttt{-no-vec -no-simd})} & \makecell{Vectorised Time [ms]\\~} & \makecell{Speed-up\\~} \\
+ \hline
+ COSMA-5 & \texttt{-xAVX} & $0.56$ & $0.25$ & 2.24x \\
+ Hamilton & \texttt{-xCORE-AVX2} & $0.49$ & $0.20$ & 2.43x \\
+ Kyll & \texttt{-xMIC-AVX512} & $1.98$ & $0.49$ & 4.07x \\
+ \hline
+ \hline
+ \end{tabular}
+\end{table}
+
+The newer and extended instruction sets show larger speed-ups compared to AVX. This is the result of:
+
+\begin{itemize}
+ \item The raw interactions being faster (Table~\ref{table:raw_interaction_results}),
+ \item The dedicated masking instructions,
+ \item The FMAs that enter the distance calculation and,
+ \item In the case of AVX-512, the larger vector lanes.
+\end{itemize}
+
+We finally note that a naive implementation of a double {\tt for} loop over all particles (See Section~\ref{sec:pVl}), interacting all particles within range without using any clever algorithms, runs in 24.49ms on the COSMA-5 system. Even if this implementation were to be sped-up using SIMD instructions by the ideal factor of 8 for AVX, this code would still be slower than our pseudo-Verlet list implementation by more than a factor of 12x. This demonstrates the importance of using clever algorithms, and investing the effort in modifying them for improved SIMD vectorization.
+
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+% Conclusions %
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+\section{Conclusions}
+
+We presented an efficient SIMD implementation of the pseudo-Verlet list algorithm commonly used in particle-based codes to interact particles located in neighbouring cells. A particle cache in sorted order alongside an accurate estimation of the upper bounds of the loop trip count were used to reduce the number of distance calculations to perform and ensure optimal data alignments. An accumulator vector was used to temporarily store the results before pushing back to memory once all neighbour interactions of a given particle were performed.
+
+When implemented in the \swift code using the AVX, AVX2 and AVX-512 instruction sets this algorithm reached speed-ups of 2.24x, 2.43x and 4.07x respectively when compared to a scalar version. These results demonstrate the importance of, not just hand-coding vectorized assembly loops, but also of developing better algorithms alongside vectorization to achieve maximal performance.
+
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+% Acknowledgement %
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+\section{Acknowledgements}
+This work would not have been possible without Lydia Heck's help and expertise. We thank the \swift team for their help and input on this project as well as John Pennycook and Georg Zitzelberger from {\sc Intel} for their help with details of the intrinsics. This work is supported by {\sc Intel} through establishment of the ICC as an {\sc Intel} parallel computing centre (IPCC). This work used the DiRAC Data Centric system at Durham University, operated by the Institute for Computational Cosmology on behalf of the STFC DiRAC HPC Facility (\url{www.dirac.ac.uk}). This equipment was funded by BIS National E-infrastructure capital grant ST/K00042X/1, STFC capital grants ST/H008519/1 and ST/K00087X/1, STFC DiRAC Operations grant ST/K003267/1 and Durham University. DiRAC is part of the National E-Infrastructure. This work made use of the facilities of the Hamilton HPC Service of Durham University.
+
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+% References %
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+\bibliographystyle{ieeetr}
+\bibliography{references}
+
+\end{document}
diff --git a/theory/Papers/Parco_2017/references.bib b/theory/Papers/Parco_2017/references.bib
new file mode 100644
index 0000000000000000000000000000000000000000..179026bb3b125a5a48bc687e72c4b7b2d4a9f4fb
--- /dev/null
+++ b/theory/Papers/Parco_2017/references.bib
@@ -0,0 +1,195 @@
+@article {ref:PG_cell_orientations,
+ author = {Gonnet, Pedro},
+ title = {A simple algorithm to accelerate the computation of non-bonded interactions in cell-based molecular dynamics simulations},
+ journal = {Journal of Computational Chemistry},
+ volume = {28},
+ number = {2},
+ publisher = {Wiley Subscription Services, Inc., A Wiley Company},
+ issn = {1096-987X},
+ url = {http://dx.doi.org/10.1002/jcc.20563},
+ doi = {10.1002/jcc.20563},
+ pages = {570--573},
+ keywords = {molecular dynamics, cell list, neighbor list},
+ year = {2007},
+}
+
+@article{ref:Verlet_list,
+ title = {Computer "Experiments" on Classical Fluids. I. Thermodynamical Properties of Lennard-Jones Molecules},
+ author = {Verlet, Loup},
+ journal = {Phys. Rev.},
+ volume = {159},
+ issue = {1},
+ pages = {98--103},
+ numpages = {0},
+ year = {1967},
+ month = {Jul},
+ publisher = {American Physical Society},
+ doi = {10.1103/PhysRev.159.98},
+ url = {https://link.aps.org/doi/10.1103/PhysRev.159.98}
+}
+
+@article{ref:Cell_list,
+title = "New method for searching for neighbors in molecular dynamics computations",
+journal = "Journal of Computational Physics",
+volume = "13",
+number = "3",
+pages = "430 - 432",
+year = "1973",
+note = "",
+issn = "0021-9991",
+doi = "http://dx.doi.org/10.1016/0021-9991(73)90046-6",
+url = "http://www.sciencedirect.com/science/article/pii/0021999173900466",
+author = "B Quentrec and C Brot",
+}
+
+@book{ref:Cell_linked_list,
+ title={Computer simulation of liquids},
+ author={Allen, M.P. and Tildesley, D.J.},
+ isbn={9780198553755},
+ lccn={87001555},
+ series={Oxford science publications},
+ url={https://books.google.co.uk/books?id=ibURAQAAIAAJ},
+ year={1987},
+ publisher={Clarendon Press}
+}
+
+@inproceedings{ref:SWIFT_PASC,
+ author = {Schaller, Matthieu and Gonnet, Pedro and Chalk, Aidan B. G. and Draper, Peter W.},
+ title = {SWIFT: Using Task-Based Parallelism, Fully Asynchronous Communication, and Graph Partition-Based Domain Decomposition for Strong Scaling on More Than 100,000 Cores},
+ booktitle = {Proceedings of the Platform for Advanced Scientific Computing Conference},
+ series = {PASC '16},
+ year = {2016},
+ isbn = {978-1-4503-4126-4},
+ location = {Lausanne, Switzerland},
+ pages = {2:1--2:10},
+ articleno = {2},
+ numpages = {10},
+ url = {http://doi.acm.org/10.1145/2929908.2929916},
+ doi = {10.1145/2929908.2929916},
+ acmid = {2929916},
+ publisher = {ACM},
+ address = {New York, NY, USA},
+ keywords = {Asynchronous data transfer, Cosmology, Extreme scaling, Fluid dynamics, Physics, Smooth Particle Hydrodynamics, Task-based parallelism},
+}
+
+@article{ref:PG_Pseudo_Verlet_list,
+ author = {Pedro Gonnet},
+ title = {Pseudo-Verlet lists: a new, compact neighbour list representation},
+ journal = {Molecular Simulation},
+ volume = {39},
+ number = {9},
+ pages = {721-727},
+ year = {2013},
+ doi = {10.1080/08927022.2012.762097},
+
+ URL = {
+http://dx.doi.org/10.1080/08927022.2012.762097
+
+ },
+ eprint = {
+http://dx.doi.org/10.1080/08927022.2012.762097
+
+ }
+
+}
+
+@article{ref:SIMD_Pair_interactions,
+ author = {{P{\'a}ll}, S. and {Hess}, B.},
+ title = "{A flexible algorithm for calculating pair interactions on SIMD architectures}",
+ journal = {Computer Physics Communications},
+ archivePrefix = "arXiv",
+ eprint = {1306.1737},
+ primaryClass = "physics.comp-ph",
+ year = 2013,
+ month = dec,
+ volume = 184,
+ pages = {2641-2650},
+ doi = {10.1016/j.cpc.2013.06.003},
+ adsurl = {http://adsabs.harvard.edu/abs/2013CoPhC.184.2641P},
+ adsnote = {Provided by the SAO/NASA Astrophysics Data System}
+}
+
+@article{ref:Mod_cell_linked_list,
+ title = "Near-neighbor calculations using a modified cell-linked list method",
+ journal = "Computer Physics Communications",
+ volume = "119",
+ number = "2",
+ pages = "135 - 148",
+ year = "1999",
+ note = "",
+ issn = "0010-4655",
+ doi = "http://dx.doi.org/10.1016/S0010-4655(98)00203-3",
+ url = "http://www.sciencedirect.com/science/article/pii/S0010465598002033",
+ author = "William Mattson and Betsy M. Rice",
+
+}
+
+@ARTICLE{ref:SPH_review,
+ author = {{Price}, D.~J.},
+ title = "{Smoothed particle hydrodynamics and magnetohydrodynamics}",
+ journal = {Journal of Computational Physics},
+archivePrefix = "arXiv",
+ eprint = {1012.1885},
+ primaryClass = "astro-ph.IM",
+ year = 2012,
+ month = feb,
+ volume = 231,
+ pages = {759-794},
+ doi = {10.1016/j.jcp.2010.12.011},
+ adsurl = {http://adsabs.harvard.edu/abs/2012JCoPh.231..759P},
+ adsnote = {Provided by the SAO/NASA Astrophysics Data System}
+}
+@article{ref:SWIFT_SIAM,
+ title={Efficient and scalable algorithms for smoothed particle hydrodynamics on hybrid shared/distributed-memory architectures},
+ author={Gonnet, Pedro},
+ journal={SIAM Journal on Scientific Computing},
+ volume={37},
+ number={1},
+ pages={C95--C121},
+ year={2015},
+ publisher={SIAM}
+}
+
+@Article{ref:FFTW,
+ author = {Frigo, Matteo and Johnson, Steven~G.},
+ title = {The Design and Implementation of {FFTW3}},
+ journal = {Proceedings of the IEEE},
+ year = 2005,
+ volume = 93,
+ number = 2,
+ pages = {216--231},
+ note = {Special issue on ``Program Generation, Optimization, and Platform Adaptation''}
+}
+
+@article{ref:Luigi_Gadget,
+ author = {Fabio Baruffa and
+ Luigi Iapichino and
+ Nicolay J. Hammer and
+ Vasileios Karakasis},
+ title = {Performance Optimisation of Smoothed Particle Hydrodynamics Algorithms
+ for Multi/Many-Core Architectures},
+ journal = {CoRR},
+ volume = {abs/1612.06090},
+ year = {2016},
+ url = {http://arxiv.org/abs/1612.06090},
+ timestamp = {Wed, 07 Jun 2017 14:40:36 +0200},
+ biburl = {http://dblp.uni-trier.de/rec/bib/journals/corr/BaruffaIHK16},
+ bibsource = {dblp computer science bibliography, http://dblp.org}
+}
+
+@article{ref:Gadget,
+ author = "Springel, Volker",
+ title = "{The Cosmological simulation code GADGET-2}",
+ journal = "Mon. Not. Roy. Astron. Soc.",
+ volume = "364",
+ year = "2005",
+ pages = "1105-1134",
+ doi = "10.1111/j.1365-2966.2005.09655.x",
+ eprint = "astro-ph/0505010",
+ archivePrefix = "arXiv",
+ primaryClass = "astro-ph",
+}
+
+@manual{ref:intel_intrinsics_guide,
+ note = "{\url{https://software.intel.com/sites/landingpage/IntrinsicsGuide/}}"
+}
\ No newline at end of file
diff --git a/theory/Papers/Parco_2017/run.sh b/theory/Papers/Parco_2017/run.sh
new file mode 100755
index 0000000000000000000000000000000000000000..005e1d9094d30829e3af79ff6bb0aa3d589856d1
--- /dev/null
+++ b/theory/Papers/Parco_2017/run.sh
@@ -0,0 +1,6 @@
+#!/bin/bash
+
+pdflatex main.tex
+bibtex main.aux
+pdflatex main.tex
+pdflatex main.tex