Files
Jungfraujoch/image_analysis/IndexAndRefine.cpp
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leonarski_fandClaude Opus 5 16bf3408f0 Address code-review findings; make detection limits detector-driven
One changeset, developed together in response to a review of this branch, so the
files carry several of the changes at once. Full test suite passes (733 cases).

Spot finding
- Split ImageSpotFinder into Detect() (flag strong pixels - the expensive
  per-pixel pass) and ExtractSpots() (CCL + min/max-pix + resolution mask), with
  Run() = both. The per-image min-pix escalation now detects ONCE and repeats
  only the cheap extraction, instead of re-running the whole finder four times
  per frame as it did on the default path. It also keeps the winning attempt's
  spot list rather than re-extracting it, so the frame that is integrated is
  exactly the frame that was scored - which a GPU re-extract could not guarantee
  (float atomic ordering).
- spot_finding_time_s no longer swallows indexing time, and indexing_time_s now
  sums every escalation call instead of reporting only the last.

Detection limits follow the detector
- The azimuthal-integration upper q and the spot-finding high-resolution limit
  are now std::optional, in the C++ structs AND in the OpenAPI schema, and
  resolve to the detector's own maximum (DiffractionExperiment::GetDetectorMaxQ_
  recipA). Adaptive detection reads a pixel's ring from the azimuthal bins, so a
  pixel outside that q range could never be strong - the integration range
  silently bounded what detection could see, regardless of the requested
  resolution limit. Regenerated the C++ and TypeScript clients; the viewer and
  the web frontend each gained a "to detector edge" switch.

Detection defaults are now per workflow (measured, not assumed)
- Stills: adaptive detection, min-pix chosen per image, no resolution clipping.
- Rotation: fixed-threshold finder, min-pix 2, 1.5 A limit.
  On a 33-crystal rotation battery, adaptive detection helped four hard crystals
  but deterministically broke three (a lost space group, a halved indexing rate,
  a collapsed merge), and the detector-edge limit cost indexing on a strong
  rotation set (100.0 -> 96.8%). Each is still overridable by its flag, and
  --no-adaptive-spots is new.

Indexer seed escalation
- Stop escalating once a seed's lattice explains >= 90% of the seed spots.
  Previously any frame with >= 80 spots always paid three indexer calls, online
  broker included.

Merge-consistency filter
- --min-image-cc gated on a per-image CC computed BEFORE the stills partiality
  post-refinement and never refreshed; the refiner now recomputes it, so the
  reported CC describes the data that are actually merged.
- Replaced the per-call cc_mask argument with one MergeOnTheFly flag, so the
  merge, the error model and MergeStats can no longer disagree about which
  images are in (the --scale path merged unfiltered while its statistics were
  filtered).

Per-image B-factor refinement (-B) removed
- Measured on four serial-stills datasets: it is a no-op where the per-image fit
  is well conditioned and actively harmful where it is not (CC1/2 -8.1, R_meas
  +23.2 on the weakest large-cell set, whose fits hit their [-50, 200] bounds on
  14-25% of images). It had also been silently DISCARDED since the partiality
  post-refinement landed - reported but not applied. Rather than fix and keep a
  knob with no demonstrated benefit, the flag and the whole image_scale_b_factor
  chain are gone: setting, scaling fit, message field, CBOR, HDF5 write and
  read-back, per-image plot, OpenAPI enum, viewer column and checkbox, docs.
  ScaleOnTheFly no longer needs Ceres at all - the fit is a linear IRLS.
  (The Wilson per-image b_factor is a different quantity and stays.)

Stills partiality width now fits both of its components
- sigma^2 = gamma0^2 + (gamma_e*d*)^2 instead of a purely angular gamma_e*d*
  with gamma0 pinned to 0. Fitted per crystal by least squares of dist_ewald^2
  on d*^2. The angular-only width is fitted over a d*^2-dense population, so it
  was pinned by the high-resolution edge and collapsed at low d*: median
  partiality 0.008 beyond 13 A for reflections that were plainly recorded, 55%
  of them under the merge's partiality floor, and the survivors divided by those
  values - which inflated the merged low-resolution intensity scale 3.6x
  (~ +9 A^2 of apparent B). Measured on 5000 stills: the ramp flattens to 0.89x,
  no observation is dropped any more (701750 -> 716811), shell-mean CC1/2 and
  R-free improve slightly. Note CC1/2, R_meas, completeness and a B-refining
  R-free are all blind to that ramp, which is why it survived earlier validation;
  the cost is high-resolution R_meas (98.5 -> 101.9 shell-averaged).

Removed dead code from add-then-remove churn
- Prediction-time "still partiality" (unreachable: no setter), the phantom
  IndexingSettings::min_indexed_spot_fraction knob (getter, no setter - now the
  constant it always was), StillsPartialityRefine's caller-less Settings
  constructor and its reference to a long-gone env var, ProcessImage's unread
  bool return, an unused include, and a dead viewer overlay hook.

Also
- Viewer: the magnifier compared a QImage with itself, so its scene rect was set
  once ever and it could not pan into a larger dataset; the hover tail timer
  could fire after leaveEvent and resurrect the resolution readout outside the
  image.
- update_version.sh regenerated the frontend lock file BEFORE bumping the
  version (every release shipped an off-by-one lock), and did git rm/git add on
  a path that has not existed since the client moved to src/client - with no
  set -e, both failed silently.
- fpga/pcie_driver/postinstall.sh tested "[ ! occurrences > 0 ]", which is a
  redirect, not a test, so dkms add never ran.
- Unit tests for the adaptive-threshold host functions, which had none.

Co-Authored-By: Claude Opus 5 (1M context) <noreply@anthropic.com>
2026-07-27 09:07:00 +02:00

667 lines
30 KiB
C++

// SPDX-FileCopyrightText: 2025 Filip Leonarski, Paul Scherrer Institute <filip.leonarski@psi.ch>
// SPDX-License-Identifier: GPL-3.0-only
#include <limits>
#include <cstdlib>
#include "IndexAndRefine.h"
#include "bragg_integration/CalcISigma.h"
#include "geom_refinement/XtalOptimizer.h"
#include "indexing/AnalyzeIndexing.h"
#include "indexing/FFTIndexer.h"
#include "indexing/MultiLatticeSearch.h"
#include "lattice_search/LatticeSearch.h"
#include "scale_merge/ReindexAmbiguity.h"
#include "scale_merge/ScaleOnTheFly.h"
IndexAndRefine::IndexAndRefine(const DiffractionExperiment &x, IndexerThreadPool *indexer, bool retain_outcomes)
: index_ice_rings(x.GetIndexingSettings().GetIndexIceRings()),
retain_outcomes_(retain_outcomes),
experiment(x),
geom_(x.GetDiffractionGeometry()),
indexer_(indexer),
rotation_indexer_counter(x) {
if (indexer && x.IsRotationIndexing())
rotation_indexer = std::make_unique<RotationIndexer>(x, *indexer);
// Only retain the whole-run per-image reflections when a later scaling/merge pass will read them.
if (retain_outcomes_)
integration_outcome.resize(x.GetImageNum());
mosaicity.resize(x.GetImageNum(), NAN);
scale_cc.resize(x.GetImageNum(), 0);
unit_cells.resize(x.GetImageNum());
}
std::optional<float> IndexAndRefine::RotationAngle(int64_t image) const {
// Mid-exposure rotation angle for image index `image`, matching the angle used for prediction.
if (const auto g = experiment.GetGoniometer())
return g->GetAngle_deg(static_cast<float>(image)) + g->GetWedge_deg() / 2.0f;
return std::nullopt;
}
void IndexAndRefine::AddImageToRotationIndexer(DataMessage &msg) {
if (rotation_indexer)
rotation_indexer->ProcessImage(msg.number, msg.spots, RotationAngle(msg.number));
}
IndexAndRefine::IndexingOutcome IndexAndRefine::DetermineLatticeAndSymmetryRotation(DataMessage &msg) {
IndexingOutcome outcome(experiment);
if (!rotation_indexer)
return outcome;
auto result = rotation_indexer->GetLattice();
if (!result.has_value()) {
auto rot_cnt = rotation_indexer_counter.Process(msg.number);
if (rot_cnt.first)
rotation_indexer->ProcessImage(msg.number, msg.spots, RotationAngle(msg.number));
if (rot_cnt.second)
rotation_indexer->RunIndexing();
result = rotation_indexer->GetLattice();
}
if (result.has_value()) {
// For rotation indexing, indexing rate is calculated only for frames, where "global" rotation indexing solution was found
msg.indexing_result = false;
// get rotated lattice
auto gon = result->axis;
if (gon) {
const float angle_deg = gon->GetAngle_deg(msg.number) + gon->GetWedge_deg() / 2.0f;
const auto rot_to_image = gon->GetTransformationAngle(-angle_deg);
outcome.lattice_candidate = result->lattice.Multiply(rot_to_image);
outcome.extra_lattice_candidates.reserve(result->extra_lattices.size());
for (const auto &el : result->extra_lattices)
outcome.extra_lattice_candidates.push_back(el.Multiply(rot_to_image));
}
outcome.experiment.BeamX_pxl(result->geom.GetBeamX_pxl())
.BeamY_pxl(result->geom.GetBeamY_pxl())
.DetectorDistance_mm(result->geom.GetDetectorDistance_mm())
.PoniRot1_rad(result->geom.GetPoniRot1_rad())
.PoniRot2_rad(result->geom.GetPoniRot2_rad())
.Goniometer(result->axis);
outcome.symmetry.centering = result->search_result.centering;
outcome.symmetry.niggli_class = result->search_result.niggli_class;
outcome.symmetry.crystal_system = result->search_result.system;
}
return outcome;
}
IndexAndRefine::IndexingOutcome IndexAndRefine::DetermineLatticeAndSymmetry(DataMessage &msg) {
auto indexing_start_time = std::chrono::steady_clock::now();
IndexingOutcome outcome(experiment);
// Seed the indexer with the strongest few spots first and escalate to more only if that fails.
// On flooded / noisy frames (XFEL, ice) a lean high-quality seed finds the lattice far more
// reliably than the full spot list, whose many spurious peaks derail the search; on clean frames
// the lean seed already works, so nothing is lost. The FULL spot list is still used for geometry
// refinement and integration downstream, so higher-resolution accuracy is preserved. Cost is
// ~1 indexer call on frames that index cleanly, up to 3 only on the hard ones. msg.spots is
// already ordered non-ice-first, strongest-first (FilterSpotsByCount), so the prefix IS the seed.
const float idx_tol = experiment.GetIndexingSettings().GetTolerance();
const float idx_tol_sq = idx_tol * idx_tol;
constexpr float SEED_STOP_FRACTION = 0.9f; // seed explained this well -> stop escalating
IndexerResult indexer_result;
bool any_executed = false;
float best_frac = -1.0f;
for (size_t seed_cap : {size_t{30}, size_t{80}, std::numeric_limits<size_t>::max()}) {
std::vector<Coord> recip;
recip.reserve(std::min<size_t>(seed_cap, msg.spots.size()));
for (const auto &i: msg.spots) {
if (index_ice_rings || !i.ice_ring) {
recip.push_back(i.ReciprocalCoord(geom_));
if (recip.size() >= seed_cap)
break;
}
}
auto res = indexer_->Run(experiment, recip);
any_executed |= res.executed;
if (!res.lattice.empty()) {
// Keep the seed the lattice explains the largest FRACTION of: a lean clean seed a good
// lattice indexes almost fully beats a flooded seed it fits only in small part. This
// auto-selects the lean seed on noisy frames (XFEL) and the full seed where the extra spots
// are real signal (weak synchrotron) -- no per-dataset setting.
const Coord a = res.lattice[0].Vec0(), b = res.lattice[0].Vec1(), c = res.lattice[0].Vec2();
int n = 0;
for (const auto &q : recip) {
const float hf = q * a, kf = q * b, lf = q * c;
const float dh = hf - std::round(hf), dk = kf - std::round(kf), dl = lf - std::round(lf);
if (dh * dh + dk * dk + dl * dl < idx_tol_sq) ++n;
}
const float frac = recip.empty() ? 0.0f : static_cast<float>(n) / recip.size();
if (frac > best_frac) { best_frac = frac; indexer_result = std::move(res); }
// A lattice that already explains nearly the whole seed is kept whatever a larger seed
// returns: the winner is the highest explained FRACTION, and adding weaker spots almost
// always lowers it. Stop here - this is what keeps clean frames at one indexer call.
if (frac >= SEED_STOP_FRACTION)
break;
}
if (recip.size() < seed_cap) // already fed every available spot; a larger cap won't add any
break;
}
if (any_executed)
msg.indexing_result = false;
if (!indexer_result.lattice.empty()) {
auto latt = indexer_result.lattice[0];
if (latt.CalcVolume() > 1.0) {
auto sg = experiment.GetGemmiSpaceGroup();
const auto algorithm = experiment.GetIndexingAlgorithm();
const bool de_novo = (algorithm == IndexingAlgorithmEnum::FFT
|| algorithm == IndexingAlgorithmEnum::FFTW);
// If space group and cell provided => enforce that symmetry in refinement.
// If not => detect the symmetry from the lattice.
if (sg && experiment.GetUnitCell()) {
outcome.symmetry = LatticeMessage{
.centering = sg->centring_type(),
.niggli_class = 0,
.crystal_system = sg->crystal_system()
};
// Place every frame's cell in ONE consistent setting for the whole dataset:
// mixed axis orders (e.g. [78,78,38] vs [38,78,78]) index the same reflection
// as different HKLs and cannot be merged. LatticeSearch gives the conventional
// setting when its detected symmetry agrees with the user's space group. On
// noisy frames it can instead pick an alternative Bravais setting (e.g. the
// sqrt2 C-centred description of a primitive tetragonal cell,
// [78,78,38]->[110,111,38]); there:
// - FFBIDX already returns the reference setting (c-last), consistent with the
// conventional frames, so its raw lattice is safe -> use it (FFBIDX neutral);
// - de-novo indexers (FFT/FFTW) return a Niggli-primitive cell with a DIFFERENT
// axis order (c-first) that would corrupt the merge -> reject the frame.
// niggli_class is left unassigned (0): it needs the primitive cell incl.
// centering, which LatticeSearch cannot recover from a (possibly centred, e.g.
// C2) user cell. A proper primitive-cell indexing path (CrystFEL-style) is deferred.
auto sym_result = LatticeSearch(latt);
if (sym_result.system == sg->crystal_system())
outcome.lattice_candidate = sym_result.conventional;
else if (!de_novo)
outcome.lattice_candidate = latt;
// else: de-novo + symmetry mismatch -> leave unset, frame is not indexed
} else {
auto sym_result = LatticeSearch(latt);
outcome.symmetry = LatticeMessage{
.centering = sym_result.centering,
.niggli_class = sym_result.niggli_class,
.crystal_system = sym_result.system
};
outcome.lattice_candidate = sym_result.conventional;
}
// Multi-lattice search for stills: store rotations that map the reference
// lattice to each accepted extra lattice. Candidates are materialized later
// in RefineGeometryIfNeeded so they're rooted in the refined (and, for
// monoclinic, reordered) main lattice.
if (outcome.lattice_candidate && indexer_result.lattice.size() > 1) {
auto ml_latt = MultiLatticeSearch(indexer_result.lattice);
for (auto &ml : ml_latt) {
if (outcome.extra_lattice_rotations.size() >= experiment.GetIndexingSettings().GetMaxExtraLattices())
break;
outcome.extra_lattice_rotations.push_back(ml.rotation_vector);
RotMatrix rot(ml.rotation_vector.Length(), ml.rotation_vector.Normalize());
outcome.extra_lattice_candidates.push_back(outcome.lattice_candidate->Multiply(rot));
}
}
}
}
auto indexing_end_time = std::chrono::steady_clock::now();
msg.indexing_time_s = std::chrono::duration<float>(indexing_end_time - indexing_start_time).count();
return outcome;
}
namespace {
// Count spots whose fractional Miller index falls within the indexing tolerance of an integer for a
// given lattice + geometry - the "how well does this model explain the spots" score used by -r multi.
int CountIndexedSpots(const DiffractionGeometry &geom, const CrystalLattice &latt,
const std::vector<SpotToSave> &spots, float tol_sq) {
const Coord a = latt.Vec0(), b = latt.Vec1(), c = latt.Vec2();
int n = 0;
for (const auto &s : spots) {
const Coord recip = s.ReciprocalCoord(geom);
const float hf = recip * a, kf = recip * b, lf = recip * c;
const float dh = hf - std::round(hf), dk = kf - std::round(kf), dl = lf - std::round(lf);
if (dh * dh + dk * dk + dl * dl < tol_sq) ++n;
}
return n;
}
} // namespace
void IndexAndRefine::RefineGeometryIfNeeded(DataMessage &msg, IndexAndRefine::IndexingOutcome &outcome) {
if (!outcome.lattice_candidate)
return;
auto start_time = std::chrono::steady_clock::now();
XtalOptimizerData data{
.geom = outcome.experiment.GetDiffractionGeometry(),
.latt = *outcome.lattice_candidate,
.crystal_system = outcome.symmetry.crystal_system,
.min_spots = experiment.GetIndexingSettings().GetViableCellMinSpots(),
// Match the [30,150] deg bound the indexers already use (FFBIDXIndexer, FFT settings):
// the struct default [60,120] clamps a monoclinic beta outside that window (e.g. a C2
// beta near 132 deg) to the boundary, corrupting the per-frame cell refinement.
.min_angle_deg = 30.0f,
.max_angle_deg = 150.0f,
.refine_beam_center = true,
.refine_distance_mm = false,
.refine_detector_angles = false,
.refine_unit_cell = !experiment.IsRotationIndexing(),
.max_time = 0.04 // 40 ms is max allowed time for the operation
};
if (outcome.symmetry.crystal_system == gemmi::CrystalSystem::Trigonal)
data.crystal_system = gemmi::CrystalSystem::Hexagonal;
switch (experiment.GetIndexingSettings().GetGeomRefinementAlgorithm()) {
case GeomRefinementAlgorithmEnum::None:
break;
case GeomRefinementAlgorithmEnum::OrientationOnly:
XtalOptimizerRotationOnly(data, msg.spots, 0.2);
XtalOptimizerRotationOnly(data, msg.spots, 0.1);
XtalOptimizerRotationOnly(data, msg.spots, 0.05);
break;
case GeomRefinementAlgorithmEnum::BeamCenter:
if (XtalOptimizer(data, {msg.spots})) {
outcome.experiment.BeamX_pxl(data.geom.GetBeamX_pxl())
.BeamY_pxl(data.geom.GetBeamY_pxl());
outcome.beam_center_updated = true;
}
break;
case GeomRefinementAlgorithmEnum::Flex: {
// Try all three refinements per image and keep whichever indexes the most spots. Beam+cell
// refinement helps some stills but diverges on sparse spot lists (few spots, long axes),
// where it pushes a good lattice out of tolerance; scoring by indexed-spot count lets each
// image fall back to orientation-only or no refinement when refinement would hurt. Ties
// prefer less refinement (strict >, not >=) to avoid overfitting.
const float tol = experiment.GetIndexingSettings().GetTolerance();
const float tol_sq = tol * tol;
XtalOptimizerData d_none = data;
XtalOptimizerData d_orient = data;
XtalOptimizerRotationOnly(d_orient, msg.spots, 0.2);
XtalOptimizerRotationOnly(d_orient, msg.spots, 0.1);
XtalOptimizerRotationOnly(d_orient, msg.spots, 0.05);
XtalOptimizerData d_beam = data;
const bool beam_ok = XtalOptimizer(d_beam, {msg.spots});
const int s_none = CountIndexedSpots(d_none.geom, d_none.latt, msg.spots, tol_sq);
const int s_orient = CountIndexedSpots(d_orient.geom, d_orient.latt, msg.spots, tol_sq);
const int s_beam = beam_ok ? CountIndexedSpots(d_beam.geom, d_beam.latt, msg.spots, tol_sq) : -1;
if (s_beam > s_none && s_beam > s_orient) {
data = d_beam;
outcome.experiment.BeamX_pxl(data.geom.GetBeamX_pxl())
.BeamY_pxl(data.geom.GetBeamY_pxl());
outcome.beam_center_updated = true;
} else if (s_orient > s_none) {
data = d_orient;
} else {
data = d_none;
}
break;
}
}
outcome.lattice_candidate = data.latt;
if (outcome.symmetry.crystal_system == gemmi::CrystalSystem::Monoclinic)
outcome.lattice_candidate->ReorderMonoclinic();
// Rebuild extra-lattice candidates from the refined (and possibly reordered) main
// lattice so they share its cell and obtuse-beta convention.
if (!outcome.extra_lattice_rotations.empty()) {
outcome.extra_lattice_candidates.clear();
outcome.extra_lattice_candidates.reserve(outcome.extra_lattice_rotations.size());
for (const auto &rv : outcome.extra_lattice_rotations) {
RotMatrix rot(rv.Length(), rv.Normalize());
outcome.extra_lattice_candidates.push_back(outcome.lattice_candidate->Multiply(rot));
}
}
// Quick orientation-only refinement of extra lattices (stills path).
// Cell, beam center, detector geometry are taken from the first lattice.
if (!experiment.IsRotationIndexing() && !outcome.extra_lattice_candidates.empty()) {
for (auto &el : outcome.extra_lattice_candidates) {
XtalOptimizerData data_extra{
.geom = data.geom,
.latt = el,
.crystal_system = data.crystal_system,
.min_spots = experiment.GetIndexingSettings().GetViableCellMinSpots(),
.refine_beam_center = false,
.refine_distance_mm = false,
.refine_detector_angles = false,
.refine_unit_cell = false,
.refine_rotation_axis = false,
.index_ice_rings = experiment.GetIndexingSettings().GetIndexIceRings(),
.max_time = 0.02
};
XtalOptimizerRotationOnly(data_extra, msg.spots, 0.1);
el = data_extra.latt;
}
}
if (outcome.beam_center_updated) {
msg.beam_corr_x = data.beam_corr_x;
msg.beam_corr_y = data.beam_corr_y;
}
auto end_time = std::chrono::steady_clock::now();
msg.refinement_time_s = std::chrono::duration_cast<std::chrono::duration<double>>(end_time - start_time).count();
}
void IndexAndRefine::QuickPredictAndIntegrate(DataMessage &msg,
const SpotFindingSettings &spot_finding_settings,
BraggPrediction &prediction,
const BraggIntegrateFn &integrate,
const IndexAndRefine::IndexingOutcome &outcome) {
if (!outcome.lattice_candidate)
return;
CrystalLattice latt = outcome.lattice_candidate.value();
// Prediction uses each frame's OWN mosaicity/profile_radius (image-local). We deliberately do NOT
// smooth them here with a running moving average: it averaged the last N *processed* frames, whose
// order under the parallel per-image loop is thread-arrival order, making the predicted rocking
// width - and hence which reflections are integrated - non-deterministic run-to-run. Prediction only
// decides membership (a reflection on the cutoff contributes ~nothing), so the per-frame value is
// fine here. The mosaicity smoothing that actually matters - keeping the partialities of one rocking
// event consistent so they tile the curve and sum toward 1 - is done deterministically in frame
// order before the 3D combine (RotationScaleMerge), where partiality is recomputed from it.
float ewald_dist_cutoff = 0.001f;
if (msg.profile_radius)
ewald_dist_cutoff = msg.profile_radius.value() * 2.0f;
if (experiment.GetBraggIntegrationSettings().GetFixedProfileRadius_recipA())
ewald_dist_cutoff = experiment.GetBraggIntegrationSettings().GetFixedProfileRadius_recipA().value() * 3.0f;
float wedge_deg = 0.0f;
float mos_deg = 0.1f;
if (experiment.GetGoniometer().has_value()) {
// Full oscillation wedge of one frame; BraggPredictionRot halves it to the +/- half-wedge of the
// partiality erf pair (Kabsch). Passing the full increment gives a half-wedge of increment/2 -
// matching ScaleOnTheFly's RotationPartiality, so the predicted partiality is used directly there.
wedge_deg = experiment.GetGoniometer()->GetWedge_deg();
if (msg.mosaicity_deg) {
mos_deg = msg.mosaicity_deg.value();
mosaicity[msg.number] = mos_deg;
}
// Second pass of the rotation two-pass: widen the prediction to the frame-order-smoothed mosaicity
// that RotationScaleMerge fitted in the first pass. Take the MAX with this frame's own estimate so
// prediction is never NARROWER than the first pass - a too-narrow smoothed value would otherwise drop
// reflections and collapse the multiplicity. (A wider value only helps prediction cover the spot.)
if (msg.number >= 0 && msg.number < static_cast<int64_t>(prediction_mosaicity_override_.size())
&& std::isfinite(prediction_mosaicity_override_[msg.number])
&& prediction_mosaicity_override_[msg.number] > 0.0f) {
mos_deg = std::max(mos_deg, prediction_mosaicity_override_[msg.number]);
mosaicity[msg.number] = mos_deg;
}
}
IntegrationOutcome i_outcome{
.geom = outcome.experiment.GetDiffractionGeometry(),
.latt = latt,
.mosaicity_deg = mos_deg,
.image_scale_cc = msg.image_scale_cc,
};
const BraggPredictionSettings settings_prediction{
.high_res_A = experiment.GetBraggIntegrationSettings().GetDMinLimit_A(),
.ewald_dist_cutoff = ewald_dist_cutoff,
.max_hkl = 100,
// Centering is a hypothesis to confirm, not assume: with no user-fixed space group, predict
// in P so the centering-absent reflections are integrated and the space-group search can
// confirm or disprove centering (and catch a missed superstructure). A user-fixed space
// group is trusted, so reject its absences here.
.centering = experiment.GetGemmiSpaceGroup().has_value() ? outcome.symmetry.centering : 'P',
.wedge_deg = std::fabs(wedge_deg),
.mosaicity_deg = std::fabs(mos_deg),
// FWHM -> sigma; 0 when monochromatic, leaving the prediction unchanged.
.bandwidth_sigma = experiment.GetBandwidthFWHM().value_or(0.0f) / 2.3548f,
};
// Predict, then integrate with the selected integrator (box-sum or profile-fit).
auto pred_start_time = std::chrono::steady_clock::now();
auto nrefl = prediction.Calc(outcome.experiment, latt, settings_prediction);
auto pred_end_time = std::chrono::steady_clock::now();
msg.bragg_prediction_time_s = std::chrono::duration<float>(pred_end_time - pred_start_time).count();
// The engine picks box-sum vs profile-fit internally from the experiment's IntegratorMode; the
// caller's callback binds it to the right image (GPU-resident buffer, host buffer, or the assembled
// FPGA image read straight on the CPU).
auto integration_start_time = std::chrono::steady_clock::now();
i_outcome.reflections = integrate(prediction.GetReflections(), nrefl, msg.number);
msg.integrated_reflections = i_outcome.reflections.size();
auto integration_end_time = std::chrono::steady_clock::now();
msg.integration_time_s = std::chrono::duration<float>(integration_end_time - integration_start_time).count();
constexpr size_t kMaxReflections = 10000;
if (i_outcome.reflections.size() > kMaxReflections) {
// Keep only smallest d (highest resolution)
std::nth_element(i_outcome.reflections.begin(),
i_outcome.reflections.begin() + static_cast<long>(kMaxReflections),
i_outcome.reflections.end(),
[](const Reflection& a, const Reflection& b) {
return a.d < b.d;
});
i_outcome.reflections.resize(kMaxReflections);
// Optional: make output ordered by d (nice for downstream / debugging)
std::sort(i_outcome.reflections.begin(), i_outcome.reflections.end(),
[](const Reflection& a, const Reflection& b) { return a.d < b.d; });
}
CalcISigma(msg, i_outcome.reflections);
CalcWilsonBFactor(msg, i_outcome.reflections);
ScaleImage(msg, i_outcome);
// Copy reflections to outgoing message
msg.reflections = i_outcome.reflections;
// Persist the per-image result for the whole-run scaling/merge pass, unless the caller opted out
// (viewer interactive use only needs the current image, returned above via msg).
if (retain_outcomes_) {
const std::unique_lock ul(reflections_mutex);
integration_outcome[msg.number] = std::move(i_outcome);
}
}
std::optional<IndexAndRefine::IndexingOutcome>
IndexAndRefine::DetermineRefineAnalyze(DataMessage &msg, const SpotFindingSettings &spot_finding_settings) {
if (!indexer_ || !spot_finding_settings.indexing)
return std::nullopt;
IndexingOutcome outcome(experiment);
if (rotation_indexer)
outcome = DetermineLatticeAndSymmetryRotation(msg);
else
outcome = DetermineLatticeAndSymmetry(msg);
if (!outcome.lattice_candidate)
return std::nullopt;
if (experiment.GetIndexingSettings().GetGeomRefinementAlgorithm() != GeomRefinementAlgorithmEnum::None)
RefineGeometryIfNeeded(msg, outcome);
if (!outcome.lattice_candidate.has_value())
return std::nullopt;
if (!AnalyzeIndexing(msg, outcome.experiment, *outcome.lattice_candidate, outcome.extra_lattice_candidates))
return std::nullopt;
{
std::unique_lock ul(reflections_mutex);
unit_cells[msg.number] = outcome.lattice_candidate->GetUnitCell();
}
msg.lattice_type = outcome.symmetry;
return outcome;
}
void IndexAndRefine::ProcessImage(DataMessage &msg,
const SpotFindingSettings &spot_finding_settings,
BraggPrediction &prediction,
const BraggIntegrateFn &integrate) {
auto outcome = DetermineRefineAnalyze(msg, spot_finding_settings);
if (outcome && spot_finding_settings.quick_integration)
QuickPredictAndIntegrate(msg, spot_finding_settings, prediction, integrate, *outcome);
}
bool IndexAndRefine::IndexFrameOnly(DataMessage &msg, const SpotFindingSettings &spot_finding_settings) {
return DetermineRefineAnalyze(msg, spot_finding_settings).has_value();
}
std::optional<RotationIndexerResult> IndexAndRefine::FinalizeRotationIndexing() {
if (rotation_indexer) {
if (const auto latt = rotation_indexer->GetLattice())
return latt;
rotation_indexer->RunIndexing();
return rotation_indexer->GetLattice();
}
return {};
}
IndexAndRefine &IndexAndRefine::ReferenceIntensities(std::vector<MergedReflection> &reference) {
// An external reference is trusted to be in the correct hand, so use it to break the merohedral
// indexing ambiguity per image (serial stills index each crystal independently).
reindex_resolver = std::make_unique<ReindexAmbiguityResolver>(experiment, reference);
return *this;
}
void IndexAndRefine::ScaleImage(DataMessage &msg, IntegrationOutcome& outcome) {
if (!reindex_resolver)
return;
// The external reference fixes the cell/space group, breaks the indexing ambiguity and reports CCref,
// but is NEVER a scale anchor: scaling an image against a foreign dataset injects cross-dataset
// systematics and is a worse reference than the data's own merge, so scaling self-references at the
// post-measurement merge for both workflows. Rotation resolves the ambiguity globally and self-scales
// in RotationScaleMerge (ChooseReindex / ReferenceIntensityCC), so there is nothing to do per image.
// Stills resolve the merohedral ambiguity per image here (each crystal indexes in a random hand; pick
// the hand best-correlated with the reference, once and for good).
if (experiment.IsRotationIndexing())
return;
auto scaling_start_time = std::chrono::steady_clock::now();
reindex_resolver->Resolve(outcome.reflections);
auto scaling_end_time = std::chrono::steady_clock::now();
msg.image_scale_time_s = std::chrono::duration<float>(scaling_end_time - scaling_start_time).count();
}
ScalingResult IndexAndRefine::ScaleAllImages(const std::vector<MergedReflection> &reference, size_t nthreads) {
ScaleOnTheFly scaling(experiment, reference);
scaling.Scale(integration_outcome, nthreads);
scale_cc.resize(integration_outcome.size());
for (int i = 0; i < integration_outcome.size(); i++)
scale_cc.at(i) = integration_outcome[i].image_scale_cc.value_or(NAN);
return ScalingResult(integration_outcome);
}
const std::vector<float> &IndexAndRefine::GetImageCC() const {
return scale_cc;
}
const std::vector<std::optional<UnitCell> > & IndexAndRefine::GetUnitCells() const {
return unit_cells;
}
std::optional<UnitCell> IndexAndRefine::GetConsensusUnitCell() const {
const auto dist_tolerance = experiment.GetIndexingSettings().GetUnitCellDistTolerance();
const auto angle_tolerance = experiment.GetIndexingSettings().GetUnitCellAngleTolerance_deg();
if (rotation_indexer) {
auto result = rotation_indexer->GetLattice();
if (!result)
return {};
return result->lattice.GetUnitCell();
}
std::vector<UnitCell> cells;
{
std::unique_lock ul(reflections_mutex);
cells.reserve(unit_cells.size());
for (const auto &cell: unit_cells) {
if (cell && cell->is_finite())
cells.emplace_back(*cell);
}
}
if (cells.empty())
return {};
if (experiment.GetUnitCell()) {
std::vector<UnitCell> accepted;
accepted.reserve(cells.size());
for (const auto &cell: cells) {
if (cell.is_close(*experiment.GetUnitCell(), dist_tolerance, angle_tolerance))
accepted.emplace_back(cell);
}
return MeanUnitCell(accepted);
}
size_t best_count = 0;
UnitCell best_reference{};
for (const auto &ref: cells) {
size_t count = 0;
for (const auto &cell: cells) {
if (cell.is_close(ref, dist_tolerance, angle_tolerance))
++count;
}
if (count > best_count) {
best_count = count;
best_reference = ref;
}
}
if (best_count == 0)
return {};
std::vector<UnitCell> accepted;
accepted.reserve(best_count);
for (const auto &cell: cells) {
if (cell.is_close(best_reference, dist_tolerance, angle_tolerance))
accepted.emplace_back(cell);
}
return MeanUnitCell(accepted);
}
std::vector<IntegrationOutcome> &IndexAndRefine::GetIntegrationOutcome() {
return integration_outcome;
}
const std::vector<IntegrationOutcome> &IndexAndRefine::GetIntegrationOutcome() const {
return integration_outcome;
}
void IndexAndRefine::ForceRotationIndexerLattice(const CrystalLattice &lattice) {
if (rotation_indexer)
rotation_indexer->ForceLattice(lattice);
}
void IndexAndRefine::ForceRotationIndexerResult(const RotationIndexerResult &result) {
if (rotation_indexer)
rotation_indexer->ForceResult(result);
}