The rc178 branch continued after #88 was squash-merged; this is its content fromb9ada7914(the tree #88 squashed) to094eee31a, as one change on main. The individual commits stay on the rc178 branch: - still battery: --cold evicts each set's input from the page cache; Alvra pixel masks; manifest fixes - AGIPD: converter to one rigid panel per module, int16 photons, mask folded in; still battery reads the converted sets - DetectorModules: panel look-up by id, plane -> panel, plane bounds and a per-pixel walk; mask size checked - tests: [PanelLayout] equivalence harness, stacked vs assembled panel layout - Dense per-pixel maps through the panel table (panel layout stage 1) - Panel id on spots and the panel table in the start message - Viewer and preview show a panel detector as it lies on the detector plane - Panel layout stage 3: per-panel spot finding (CPU+GPU, CCL) and raster algorithms on the plane raster - Panel layout stage 2: prediction and Bragg integration through the panel table - XTC reader: frames handed up as stored, streams indexed in parallel - XFEL reader: integer frames stay integer, one gain, placement by panel - EXTERNAL_TEST_DATA_STILLS.md: images used vs the entry for every set; drop "Not in the battery" - still battery: EuXFEL sets read the depositors' Cheetah CXI files directly; AGIPD converter removed - float32_to_int16.py: a non-finite pixel becomes -32768, the int16 error marker, not a zero count - CrystFEL geometry: read the pixel masks and bad regions instead of ignoring them - Panel layout stage 5: the XFEL reader hands up the stored frame and its panel table - Panel table persisted in NXmx; modulation grid and pre-scan memo key on the plane - still battery: Alvra sets take their pixel mask from the CrystFEL geometry, not --mask-good - still battery: take the deposited model as mmCIF where the RCSB has no PDB-format file - still battery: dimple gets PDB-format coordinates converted from an mmCIF-only deposition - stills fixed cost: geometry refinement and pre-scan do the same work in less wall time - stills geometry sample and trial spot finding run as many workers as the image pass - Stills integration: background ring reach measured on empty apertures, radial curvature from the whole frame - StillsPartialityRefine: the partiality width is the run's, measured on the crystals, not the prediction window's - MergeOnTheFly: capture term and multiplicative outlier band for the stills merge (both opt-in) - Stills given a cell: the written cell is the mean over the frames that are merged - Stills: the radial curvature correction decided per run on the same empty apertures - StillsPartialityRefine: measure the run width only on shells with signal - Stills pre-scan: report the paired z of the radial-correction comparison - module placement: the five concurrent fits each keep every thread - still battery: score R-free against the deposited data through the same dimple protocol - still battery: the R-free target is the lower of the deposition's dimple and published values - Stills: background clip follows the radial curve; signal disk from the lattice spacing - Stills keep an overloaded observation as a lower bound instead of dropping it - Stills: drop the lattice-spacing signal disk; the correction decision back on the plain clip - battery: R-free against the deposition without refinement only, one protocol for rotation and stills - still battery: EuXFEL sets run on a 2,000-image subset for now - stills geometry refinement: fit the detector distance and the cell together - stills geometry refinement: a distance given with --detector-distance is held in the joint fit - Metal integration engine: back to its panel-s5 kernels; Mac stills keep the old clip, no saturation count - Metal integration test: the CPU comparison runs on a rotation experiment - Stills: kept overloads go back to the drop where they are not concentrated at low resolution - stills distance search: an absolute 30-3000 mm scan, a sample found without d-limits, the fit iterated - battery results: XFEL still battery 20261022-1358 on rc1780cf62452c- 12 sets, cold, R_free unrefined - battery results: still summary gains the resolution of our merge and of the deposition - Pre-scan masks a pixel at the saturation limit on most frames, as one holding the error value - Stills keep an overload as a lower bound only where it has pixels at the limit; run-level gate removed - XFEL reader: a per-frame mask is read the way the frames are, its chunk inflated outside the HDF5 lock - stills distance search: every centre scanned with a wider acceptance, a larger sample where nothing indexes - rugnux usage: --beam-center-check describes the absolute 30-3000 mm stills distance scan, not the old 60-160 % grid - stills: detector tilt refined in the geometry pre-pass, kept where held-out frames agree - CLAUDE.md: the changelog is written once, just before the merge into main - condensed one-liners of what users get - broker: serve the placed model and its maps of the last rugnux live run (/rugnux/model.cif, /rugnux/map.ccp4) - frontend: Mol* viewer of the placed model and its density on the Rugnux live page - writer: _model.cif from rugnux live keeps the input model's metadata, as the served model.cif does - rugnux live maps: one unit cell centred on the model; the viewer opens on all of it - Anomalous difference map: ANOM/PHANOM in _maps.mtz, /rugnux/map.ccp4?type=anom, a magenta mesh in the viewer - Mol* viewer: open with the maps drawn within 10 A of the centre of view - Mol* viewer: aaredb's structure-viewer setup, on a black stage - rugnux: the gain of a stills file that states none is read off its single-photon peak where the background resolves photons - Mol* viewer: in line with AareDB's StructureView at its current head (8ece2c2) - ACKNOWLEDGEMENT: the web frontend's Mol* viewer follows AareDB's setup (G. Gotthard, PSI) - stills tilt decision: the modules stay where the run placed them - still battery: no distance pins and no per-set tuning flags; gain from the data except where a file's baseline hides it - battery results: rc178 6f6f69 - full still battery and full rotation battery with REFMAC - Bragg integration: a CCD rotation sweep's sigmas at the measured gain, intensities in photons - BackgroundGain: the gain of a frame that resolves photons is the spacing of its photon peaks, so a baseline left in the frame no longer hides it - ShadowFinder: measure the background's azimuthal modulation instead of predicting it from the polarization - BackgroundGain: one gain estimate for rotation and stills; the still battery no longer gives EuXFEL 152 its gain - ShadowFinder: measure the modulation robustly under a wide one-sided shadow - ShadowFinderTest: a one-sided shadow is not fitted as part of the background's modulation - ShadowFinder: back to the predicted polarization factor, in the plane the background shows - MXAnalysisAfterFPGA: the Bragg engine's edge mask in the image's layout, so raw / untransformed FPGA runs start again - battery results: still battery on rc178 e54f55 replaces the earlier rc178 still tables - XFELReader: per-frame mask and photon conversion without a library call or a branch per pixel - stills geometry trial: the hypotheses a search asks are indexed side by side - stills tilt decision: the fits start beside the pre-scan and the geometry trial - XFELReader: a deflated frame is inflated and converted a piece at a time, while it is in the cache - XFELReader: a byte-shuffled frame is unshuffled a piece at a time, a whole pixel per step - GeometryRefiner: residuals carry only the blocks a fit moves; beam and distance one block - GeometryRefiner: a spot's residual differentiates its observed and predicted halves apart - docs: EXTERNAL_TEST_DATA lists every open-arm battery set, with corrected values and counts - battery: doc_check.py cross-checks the manifests against the dataset pages - stills module placement: the placement fit gets half the threads, each held-out fit an eighth - still battery: the EuXFEL sets run on all their frames, as the published still runs did - battery results: still battery on rc178 a0ce6c, cold on a quiet machine, replaces the earlier rc178 table - macOS build: explicit size_t in the XFEL reader's row bounds; parentheses in the CPU preprocessor's select Co-Authored-By: Claude Opus 5.5 <noreply@anthropic.com> Claude-Session: https://claude.ai/code/session_015CeEGgpKdfkCTJb3YNMJcu
293 lines
13 KiB
C++
293 lines
13 KiB
C++
// SPDX-FileCopyrightText: 2024 Filip Leonarski, Paul Scherrer Institute <filip.leonarski@psi.ch>
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// SPDX-License-Identifier: GPL-3.0-only
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#include "HDF5DataFilePluginMX.h"
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inline std::string to_bravais_code(const std::optional<LatticeMessage> &lm_opt) {
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if (!lm_opt.has_value()) return "";
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const auto &lm = lm_opt.value();
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const char C = lm.centering;
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switch (lm.crystal_system) {
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case gemmi::CrystalSystem::Triclinic:
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if (C == 'P') return "aP";
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break;
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case gemmi::CrystalSystem::Monoclinic:
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if (C == 'P') return "mP";
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if (C == 'A') return "mA";
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if (C == 'B') return "mB";
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if (C == 'C') return "mC";
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break;
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case gemmi::CrystalSystem::Orthorhombic:
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if (C == 'P') return "oP";
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if (C == 'A') return "oA";
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if (C == 'B') return "oB";
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if (C == 'C') return "oC";
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if (C == 'F') return "oF";
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if (C == 'I') return "oI";
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break;
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case gemmi::CrystalSystem::Tetragonal:
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if (C == 'P') return "tP";
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if (C == 'I') return "tI";
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break;
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case gemmi::CrystalSystem::Trigonal:
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if (C == 'R') return "hR"; // rhombohedral in hex setting
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break;
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case gemmi::CrystalSystem::Hexagonal:
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if (C == 'P') return "hP";
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break;
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case gemmi::CrystalSystem::Cubic:
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if (C == 'P') return "cP";
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if (C == 'F') return "cF";
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if (C == 'I') return "cI";
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break;
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}
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return "";
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}
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HDF5DataFilePluginMX::HDF5DataFilePluginMX(const StartMessage &msg)
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: max_spots(msg.max_spot_count),
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max_extra_lattices(msg.max_extra_lattices),
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indexing(msg.indexing_algorithm != IndexingAlgorithmEnum::None) {
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}
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void HDF5DataFilePluginMX::OpenFile(HDF5File &data_file, const DataMessage &msg, size_t images_per_file) {
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bkg_estimate.reserve(images_per_file);
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ice_ring_score.reserve(images_per_file);
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spindle_blind_fraction.reserve(images_per_file);
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if (max_spots == 0)
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return;
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spot_x.reserve(max_spots * images_per_file);
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spot_y.reserve(max_spots * images_per_file);
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spot_int.reserve(max_spots * images_per_file);
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spot_ice_ring.reserve(max_spots * images_per_file);
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spot_h.reserve(max_spots * images_per_file);
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spot_k.reserve(max_spots * images_per_file);
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spot_l.reserve(max_spots * images_per_file);
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spot_dist_ewald.reserve(max_spots * images_per_file);
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spot_panel.reserve(max_spots * images_per_file);
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if (indexing) {
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spot_indexed.reserve(max_spots * images_per_file);
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spot_lattice.reserve(max_spots * images_per_file);
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indexed_lattice.reserve(images_per_file * 9);
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extra_lattices.reserve(images_per_file * max_extra_lattices * 9);
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}
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beam_corr_x.reserve(images_per_file);
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beam_corr_y.reserve(images_per_file);
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npeaks.reserve(images_per_file);
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strong_pixel_count.reserve(images_per_file);
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indexed.reserve(images_per_file);
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profile_radius.reserve(images_per_file);
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mosaicity_deg.reserve(images_per_file);
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b_factor.reserve(images_per_file);
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resolution_estimate.reserve(images_per_file);
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spot_count_total.reserve(images_per_file);
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spot_count_ice.reserve(images_per_file);
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spot_count_ice_control.reserve(images_per_file);
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spot_count_indexed.reserve(images_per_file);
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spot_count_low_res.reserve(images_per_file);
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integrated_reflections.reserve(images_per_file);
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image_scale_factor.reserve(images_per_file);
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image_scale_cc.reserve(images_per_file);
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image_scale_mosaicity.reserve(images_per_file);
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}
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void HDF5DataFilePluginMX::Write(const DataMessage &msg, uint64_t image_number) {
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if (msg.bkg_estimate.has_value())
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bkg_estimate[image_number] = msg.bkg_estimate.value();
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if (msg.ice_ring_score.has_value())
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ice_ring_score[image_number] = msg.ice_ring_score.value();
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if (msg.spindle_blind_fraction.has_value())
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spindle_blind_fraction[image_number] = msg.spindle_blind_fraction.value();
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if (max_spots == 0)
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return;
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if (image_number >= max_image_number) {
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max_image_number = image_number;
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spot_x.resize(max_spots * (max_image_number + 1));
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spot_y.resize(max_spots * (max_image_number + 1));
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spot_int.resize(max_spots * (max_image_number + 1));
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spot_ice_ring.resize(max_spots * (max_image_number + 1));
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spot_h.resize(max_spots * (max_image_number + 1));
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spot_k.resize(max_spots * (max_image_number + 1));
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spot_l.resize(max_spots * (max_image_number + 1));
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spot_lattice.resize(max_spots * (max_image_number + 1), -1);
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spot_dist_ewald.resize(max_spots * (max_image_number + 1), NAN);
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spot_panel.resize(max_spots * (max_image_number + 1), -1);
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if (indexing) {
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spot_indexed.resize(max_spots * (max_image_number + 1));
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indexed_lattice.resize((max_image_number + 1) * 9, NAN);
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extra_lattices.resize((max_image_number + 1) * max_extra_lattices * 9, NAN);
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}
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}
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uint32_t spot_cnt = std::min(msg.spots.size(), max_spots);
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for (int i = 0; i < spot_cnt; i++) {
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spot_x[max_spots * image_number + i] = msg.spots[i].x;
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spot_y[max_spots * image_number + i] = msg.spots[i].y;
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spot_int[max_spots * image_number + i] = msg.spots[i].intensity;
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spot_panel[max_spots * image_number + i] = msg.spots[i].panel;
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if (msg.spots[i].panel >= 0)
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spot_panel_present = true;
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if (indexing) {
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spot_indexed[max_spots * image_number + i] = msg.spots[i].indexed;
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spot_lattice[max_spots * image_number + i] = msg.spots[i].lattice;
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spot_h[max_spots * image_number + i] = msg.spots[i].h;
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spot_k[max_spots * image_number + i] = msg.spots[i].k;
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spot_l[max_spots * image_number + i] = msg.spots[i].l;
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spot_dist_ewald[max_spots * image_number + i] = msg.spots[i].dist_ewald_sphere;
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}
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spot_ice_ring[max_spots * image_number + i] = msg.spots[i].ice_ring;
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}
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npeaks[image_number] = spot_cnt;
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strong_pixel_count[image_number] = msg.strong_pixel_count.value_or(0);
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spot_count_total[image_number] = msg.spot_count.value_or(0);
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spot_count_ice[image_number] = msg.spot_count_ice_rings.value_or(0);
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spot_count_ice_control[image_number] = msg.spot_count_ice_control.value_or(NAN);
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spot_count_low_res[image_number] = msg.spot_count_low_res.value_or(0);
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if (indexing) {
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indexed[image_number] = msg.indexing_result.value_or(0);
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// Fallback value is indexing result (1 or 0 lattices)
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indexing_lattice_count[image_number] = msg.indexing_lattice_count.value_or(indexed[image_number]);
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profile_radius[image_number] = msg.profile_radius.value_or(NAN);
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mosaicity_deg[image_number] = msg.mosaicity_deg.value_or(NAN);
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b_factor[image_number] = msg.b_factor.value_or(NAN);
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resolution_estimate[image_number] = msg.resolution_estimate.value_or(NAN);
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beam_corr_x[image_number] = msg.beam_corr_x.value_or(NAN);
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beam_corr_y[image_number] = msg.beam_corr_y.value_or(NAN);
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spot_count_indexed[image_number] = msg.spot_count_indexed.value_or(0);
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integrated_reflections[image_number] = msg.integrated_reflections.value_or(0);
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if (msg.indexing_lattice) {
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auto tmp = msg.indexing_lattice->GetVector();
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for (int i = 0; i < 9; i++)
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indexed_lattice[image_number * 9 + i] = tmp[i];
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} else {
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for (int i = 0; i < 9; i++)
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indexed_lattice[image_number * 9 + i] = NAN;
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}
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for (size_t li = 0; li < max_extra_lattices; li++) {
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const size_t base = (image_number * max_extra_lattices + li) * 9;
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if (li < msg.indexing_extra_lattices.size()) {
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auto tmp = msg.indexing_extra_lattices[li].GetVector();
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for (int i = 0; i < 9; i++)
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extra_lattices[base + i] = tmp[i];
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} else {
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for (int i = 0; i < 9; i++)
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extra_lattices[base + i] = NAN;
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}
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}
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if (msg.lattice_type) {
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bravais_lattice[image_number] = to_bravais_code(msg.lattice_type);
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niggli_class[image_number] = msg.lattice_type->niggli_class;
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} else {
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bravais_lattice[image_number] = "";
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niggli_class[image_number] = 0;
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}
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if (msg.image_scale_factor.has_value())
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image_scale_present = true;
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image_scale_factor[image_number] = msg.image_scale_factor.value_or(NAN);
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image_scale_cc[image_number] = msg.image_scale_cc.value_or(NAN);
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image_scale_mosaicity[image_number] = msg.image_scale_mosaicity.value_or(NAN);
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}
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}
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void HDF5DataFilePluginMX::WriteFinal(HDF5File &data_file) {
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HDF5Group(data_file, "/entry/MX").NXClass("NXcollection");
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if (!spot_x.empty()) {
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data_file.SaveVector("/entry/MX/peakXPosRaw", spot_x, {(hsize_t) (max_image_number + 1), max_spots});
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data_file.SaveVector("/entry/MX/peakYPosRaw", spot_y, {(hsize_t) (max_image_number + 1), max_spots});
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data_file.SaveVector("/entry/MX/peakTotalIntensity", spot_int, {(hsize_t) (max_image_number + 1), max_spots});
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data_file.SaveVector("/entry/MX/peakIceRingRes", spot_ice_ring, {(hsize_t) (max_image_number + 1), max_spots});
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data_file.SaveVector("/entry/MX/nPeaks", npeaks.vec());
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if (spot_panel_present)
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data_file.SaveVector("/entry/MX/peakPanel", spot_panel, {(hsize_t) (max_image_number + 1), max_spots});
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if (indexing) {
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data_file.SaveVector("/entry/MX/peakH", spot_h, {(hsize_t) (max_image_number + 1), max_spots});
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data_file.SaveVector("/entry/MX/peakK", spot_k, {(hsize_t) (max_image_number + 1), max_spots});
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data_file.SaveVector("/entry/MX/peakL", spot_l, {(hsize_t) (max_image_number + 1), max_spots});
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data_file.SaveVector("/entry/MX/peakDistEwaldSphere", spot_dist_ewald,
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{(hsize_t) (max_image_number + 1), max_spots});
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data_file.SaveVector("/entry/MX/peakIndexed", spot_indexed, {(hsize_t) (max_image_number + 1), max_spots});
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data_file.SaveVector("/entry/MX/peakLattice", spot_lattice, {(hsize_t) (max_image_number + 1), max_spots});
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}
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}
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if (!strong_pixel_count.empty())
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data_file.SaveVector("/entry/MX/strongPixels", strong_pixel_count.vec());
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if (!spot_count_ice.empty())
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data_file.SaveVector("/entry/MX/peakCountIceRingRes", spot_count_ice.vec());
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if (!spot_count_ice_control.empty())
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data_file.SaveVector("/entry/MX/peakCountIceRingControl", spot_count_ice_control.vec());
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if (!spot_count_indexed.empty())
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data_file.SaveVector("/entry/MX/peakCountIndexed", spot_count_indexed.vec());
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if (!spot_count_low_res.empty())
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data_file.SaveVector("/entry/MX/peakCountLowRes", spot_count_low_res.vec());
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if (!spot_count_total.empty())
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data_file.SaveVector("/entry/MX/peakCountUnfiltered", spot_count_total.vec());
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if (!indexed.empty())
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data_file.SaveVector("/entry/MX/imageIndexed", indexed.vec());
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if (!indexing_lattice_count.empty())
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data_file.SaveVector("/entry/MX/indexingLatticeCount", indexing_lattice_count.vec());
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if (!indexed_lattice.empty())
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data_file.SaveVector("/entry/MX/latticeIndexed", indexed_lattice, {(hsize_t) (max_image_number + 1), 9})
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->Units("Angstrom");
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if (!extra_lattices.empty())
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data_file.SaveVector("/entry/MX/latticeIndexedExtra", extra_lattices,
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{(hsize_t) (max_image_number + 1), (hsize_t) max_extra_lattices, 9})
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->Units("Angstrom");
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if (!bkg_estimate.empty())
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data_file.SaveVector("/entry/MX/bkgEstimate", bkg_estimate.vec());
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if (!ice_ring_score.empty())
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data_file.SaveVector("/entry/MX/iceRingScore", ice_ring_score.vec());
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if (!spindle_blind_fraction.empty())
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data_file.SaveVector("/entry/MX/spindleBlindFraction", spindle_blind_fraction.vec());
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if (!profile_radius.empty())
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data_file.SaveVector("/entry/MX/profileRadius", profile_radius.vec())->Units("Angstrom^-1");
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if (!mosaicity_deg.empty())
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data_file.SaveVector("/entry/MX/mosaicity", mosaicity_deg.vec())->Units("deg");
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if (!b_factor.empty())
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data_file.SaveVector("/entry/MX/bFactor", b_factor.vec())->Units("Angstrom^2");
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if (!beam_corr_x.empty())
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data_file.SaveVector("/entry/MX/beam_corr_x", beam_corr_x.vec())->Units("pixel");
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if (!beam_corr_y.empty())
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data_file.SaveVector("/entry/MX/beam_corr_y", beam_corr_y.vec())->Units("pixel");
|
|
if (!niggli_class.empty())
|
|
data_file.SaveVector("/entry/MX/niggliClass", niggli_class.vec());
|
|
if (!bravais_lattice.empty())
|
|
data_file.SaveVector("/entry/MX/bravaisLattice", bravais_lattice.vec());
|
|
if (!resolution_estimate.empty())
|
|
data_file.SaveVector("/entry/MX/resolutionEstimate", resolution_estimate.vec())->Units("Angstrom");
|
|
if (!integrated_reflections.empty())
|
|
data_file.SaveVector("/entry/MX/integratedReflections", integrated_reflections.vec());
|
|
|
|
if (image_scale_present) {
|
|
data_file.SaveVector("/entry/MX/imageScaleFactor", image_scale_factor.vec());
|
|
data_file.SaveVector("/entry/MX/imageScaleCC", image_scale_cc.vec());
|
|
data_file.SaveVector("/entry/MX/imageScaleMosaicity", image_scale_mosaicity.vec())->Units("deg");
|
|
}
|
|
}
|