18 Commits

Include renames

Author	SHA1	Message	Date
leonarski_fandClaude Opus 5	83e95b0c5a	indexing: stop computing angles the candidate filter only compares ... Candidate cell filtering called acos three times per candidate to turn dot products into degrees, then compared those against the min/max angle bounds. acos is strictly decreasing on [-1, 1], so "angle outside [min, max]" is exactly "cosine outside [cos(max), cos(min)]" with the ends swapped - the bounds convert once, and the three acos calls per candidate disappear. The same loop also re-derived every already-accepted candidate's unit cell on each new triple, inside the duplicate scan: three more acos each, for every candidate accepted so far. Those cells are now kept alongside the candidates. Measured on de-novo serial stills, where the indexer runs once per image: 34.43 s -> 14.17 s on one dataset and 21.92 s -> 6.59 s on another, with the indexing rate and the merged reflection count unchanged (one gained 0.25 points of indexing rate). acos had been 40% of the whole process there. Scope is narrower than that number suggests, and worth stating: the win is on the de-novo path, which Auto selects for stills only when NO cell is known. With a known cell Auto picks ffbidx, which reaches the same filter but feeds it few candidates - measured neutral there (+0.5% instructions, -1.6% wall, identical output), and that path already runs 14x faster in absolute terms. Rotation runs the indexer twice per dataset rather than per image, so it is unaffected: the full 37-crystal battery is identical, crystal for crystal. Comparing cosines instead of angles can only move a candidate that sits on the bound, so the filter's behaviour is unchanged except at that measure-zero boundary. Co-Authored-By: Claude Opus 5 (1M context) <noreply@anthropic.com>	2026-08-02 21:24:57 +02:00
leonarski_fandClaude Opus 5	6e805f53c0	image_analysis: stop paying for work that is thrown away ... Three independent costs, each measured, none changing a result. Across the 37-crystal regression set the run time halves (median per crystal 2.0x, total 2.3x) and every crystal's merge statistics are unchanged. The image copy back from the device moved the whole preprocessed frame - 72 MB on a large detector, every frame, per worker - to serve a single host consumer that reads only the strong pixels, at most a few hundred kilobytes of it. Give the buffer a Gather() so that consumer asks for the values it actually wants (a host loop on the CPU, a small kernel on the GPU), and copy the frame back only when a CPU spot finder will genuinely read it. The copy the other way was worse: it came from an unregistered vector, so the driver staged it through its own pinned pool with a host-side memcpy on the calling thread, which does not overlap and collapses under concurrency - 11.6 GB/s at one worker, 1.6 GB/s at eight. That, not any hardware limit, is why throughput stopped improving past four to eight workers. Pinning the decompression buffer once per worker fixes it: on a 18 Mpx dataset the image loop goes from 13.6 to 7.9 ms per image at 32 workers, and 32 workers now beat 8 instead of losing to them. Ceres was computing seventeen partial derivatives where five are free. The per-image rotation refinement frees the beam and the orientation and holds distance, detector angles, rotation axis and cell constant, but the cost function declared all seven blocks, so every residual evaluated in Jet<17> arithmetic. A residual exposing only the two free blocks - the same arithmetic, the constants baked in - halves refinement, and it is exact rather than merely close: dual coordinates evolve independently, so the residuals and the free Jacobian columns are unchanged bit for bit. The merge sorted an index array with a comparator that dereferenced a 1.6 GB array of 72-byte records, i.e. a random walk over memory, single-threaded, twice per two-pass run. Sorting a packed key instead is 2.4x. French-Wilson allocated its integration scratch per reflection and ran serially; it now takes caller-owned scratch and runs over chunks, 4.2x. The correction surfaces re-tested every observation for usability and parity on each of ~22 passes and re-allocated their accumulators each time; bucket the indices once and hoist the buffers. Also convert std::round to std::rint where the rounded value only ever enters a squared residual. The tie rules differ - away from zero against to even - so this is safe exactly where a tie flips the sign but not the magnitude, and unsafe wherever the value becomes a Miller index; those sites keep std::round. Verified over all 2^32 float bit patterns: 8388608 exact ties exist, and the squared residual is bitwise equal for every one of them. Worth little on its own here, because the rounding that dominates is in candidate refinement, where the value is an index and the substitution is not available. Co-Authored-By: Claude Opus 5 (1M context) <noreply@anthropic.com>	2026-08-01 21:35:28 +02:00
leonarski_fandClaude Opus 5	0ae1a307bc	indexing: complete a rank-deficient direction set, and keep the higher-symmetry setting ... The FFT shortlist could be rank-deficient, and then no cell could be formed at all. FilterFFTResults takes the strongest max_vectors RAW directions and only then prunes ones within 5 degrees of each other, but a single lattice row is sampled by many neighbouring directions of the 16k half-sphere, so thirty raw peaks routinely prune down to four or five distinct directions - the strongest, hence shortest, rows. When a crystal's densest rows share a plane, every surviving direction is coplanar, every triple the reduction forms is degenerate, and the indexer returns nothing. On such a crystal the weak third axis was the eighth distinct direction, at raw rank 78. Keep walking the same magnitude order for up to four more directions that are 5 degrees clear of everything kept, appended after the length sort so the earlier entries hold their positions and the reduction still forms every triple it formed before - the shortlist only gains candidates at its end. That exposed two ways a change of SETTING was mistaken for a different lattice. A centred conventional cell is an exact integer multiple of its primitive one, so the same lattice described two ways differs by that factor: comparing conventional volumes reads a setting change as a sub-cell or a supercell. Both the candidate selection in the rotation indexer and the pass-2 comparison in the driver did exactly that, and between them they discarded a correctly-classified cubic F cell in favour of the body-centred tetragonal description of the very same lattice. Compare primitive volumes in both, as the scheme comparison already did. Fixing the volumes alone was not enough, because the indexed fraction is also biased across crystal systems: a subgroup setting holds fewer cell parameters fixed than its supergroup, so it can never index fewer spots and will always look better by that measure. Where a candidate has a lower lattice point-group order at the same primitive volume - the signature of the same lattice in less symmetry - require it to index markedly better, not merely better, before it displaces the incumbent. A general metric-symmetry promotion was implemented and rejected on evidence: it raised a correct body-centred orthorhombic cell to triclinic and a monoclinic one to C-centred orthorhombic, and no threshold separates the cases, because a false pseudo-orthorhombic degeneracy measured tighter than a true cubic one on obliquity and on alternative-basis axis excess alike. Metric alone cannot decide this; only the intensities can, which is what the space-group search is for. Measured over the 37-crystal regression set: one crystal goes from failing outright to 91% indexed with 91% completeness and a better R_meas than the reference, one keeps the cubic setting it had before, and every other crystal is byte-identical. Full unit suite passes. Co-Authored-By: Claude Opus 5 (1M context) <noreply@anthropic.com>	2026-08-01 12:59:34 +02:00
leonarski_f	67dca388bd	v1.0.0-rc.160 (#70) ... This is an UNSTABLE release. It includes many experimental features, as well as many AI generated fixes. We recommend using rc.152 for production use. * rugnux: Add `--model model.pdb` - score the merged data against an atomic model and compute initial maps. It reports R-work/R-free (scaling the model to the observed amplitudes with an overall scale, an anisotropic B and a flat bulk solvent - the standard few-parameter model, so a batch of maps stays directly comparable) and writes 2Fo-Fc / Fo-Fc electron-density maps (CCP4) plus a map-coefficient MTZ. The structure itself is not refined; the model is only re-fractionalised into the data cell. * rugnux: The merged reflection output now carries French-Wilson amplitudes (|F| and its sigma) next to the intensities - MTZ `F`/`SIGF`, mmCIF `_refln.F_meas_au`, and the text HKL - computed with the correct centric/acentric Wilson prior and epsilon multiplicity, so a downstream program (e.g. phenix.refine) can refine against amplitudes. The intensity columns are unchanged. * rugnux: R-free test-set flags are now assigned deterministically and consistently across symmetry - a Bijvoet pair I(+)/I(-) is never split between the work and free sets, and the assignment is a reproducible per-hkl hash that depends only on the reflection index, so every dataset of one crystal form gets the same ~5% free set (what a multi-dataset campaign such as PanDDA needs). On small data the fraction is floored so the test set stays large enough for a stable R-free (~500 reflections, capped at 10%); it stays flat at 5% on ordinary data. When a reference MTZ carries a `FreeR_flag` column its test set is imported instead, letting a whole campaign inherit one shared free set. * rugnux: A reference MTZ (`--reference-mtz`) can now fix the space group and cell for rotation data too (previously rejected), without being used to scale - the rotation merge stays self-consistent. When the crystal has an indexing (merohedral) ambiguity - a lattice symmetry higher than its Laue symmetry, e.g. P3/P4/P6/C2 - the reference also resolves it: each candidate reindexing (identity plus the twin-law cosets of the metric symmetry) is scored by its intensity correlation against the reference and the data are re-merged in the best-correlating one. This is a metric-preserving relabelling of hkl (the cell is unchanged) and a no-op for a holohedral crystal such as lysozyme. * rugnux: `--model` validation now aligns the data to the model before scoring - the observed reflections are reindexed into the model's enantiomorph when the two differ only by hand (indistinguishable from merged intensities). A merohedral indexing ambiguity is resolved against the reference MTZ when one is given (so a whole campaign shares one indexing convention); only with a model and no reference does validation fall back to fitting each candidate reindexing and keeping the lowest R-free. * rugnux: De-novo symmetry - recover a genuine high-symmetry group whose data are imperfectly scaled. Such a merge's within-orbit chi² lands just past the self-consistency bound (each real symmetry step adds a little systematic scatter), right where a merohedral twin also lands, so the chi² ratio alone cannot separate them. The candidate is now rescued when the extra intensity-proportional systematic error it invokes stays small relative to the confirmed subgroup - a genuine symmetry step gains multiplicity without inflating the merge error model's b, whereas a twin forces non-equivalent reflections together and b balloons. Fixes cubic insulin (I23 instead of I222) with no change to any other crystal in the test battery, including the twins that must stay in their lower symmetry. * Docs: Document the French-Wilson amplitude estimation, R-free flagging, reference-based space-group/ambiguity resolution, and model-based validation/maps in CPU_DATA_ANALYSIS.md. * Frontend: The status-bar pill now shows a progress bar during detector calibration (previously only during measurement), and the calibration state and its button are labelled "Calibration"/"CALIBRATE" (the internal `Pedestal` state name is unchanged for back-compatibility).Reviewed-on: #70 Co-authored-by: Filip Leonarski <filip.leonarski@psi.ch>	2026-07-19 09:39:28 +02:00
leonarski_f	d6389e12da	v1.0.0-rc.156 (#66) ... This is an UNSTABLE release. It includes many experimental features, as well as many AI generated fixes. We recommend using rc.152 for production use. * jfjoch_process: Major rotation (rot3d) data processing overhaul - robust profile-fit integration, Cauchy-loss scaling with optional absorption surface, de-novo indexing and space-group/centering determination fixes, and merging statistics + ISa in the mmCIF output. * jfjoch_process: Add EXPERIMENTAL ice-ring detection (--detect-ice-rings) that excludes ice reflections from scaling. * Compression: Add BSHUF_ZSTD_RLE_HUFF, make compression size-aware (drop frames that don't fit rather than aborting), and add the jfjoch_recompress tool. * jfjoch_viewer: Report "Multiple lattices detected" and grey out "Analyze dataset" on a live connection. * jfjoch_broker: Write smargon chi/phi goniometer positions to NXmx; read sensor thickness/material from HDF5 metadata. * CI: Build Windows (CUDA and non-CUDA) installers.Reviewed-on: #66 Co-authored-by: Filip Leonarski <filip.leonarski@psi.ch>	2026-07-03 19:18:56 +02:00
leonarski_f	75e401f0e5	v1.0.0-rc.153 (#63) ... This is an UNSTABLE release. It includes many experimental features, as well as many AI generated fixes. We recommend using rc.152 for production use. * jfjoch_broker: Add EXPERIMENTAL pixelrefine mode for image processing * jfjoch_broker: Allow to load user mask from 8-bit and 16-bit TIFF files * jfjoch_broker: Add ROI calculation in non-FPGA workflow * jfjoch_broker: Fixes to TCP image pusher * jfjoch_broker: Remove NUMA bindings * jfjoch_broker: Improvements to indexing * jfjoch_broker: For PSI EIGER, trimming energies are taken from the detector configuration (now compulsory) instead of hardcoded values * jfjoch_writer: Save ROI definitions and the per-pixel ROI bitmap in the master file; azimuthal ROIs support phi (angular) sectors * jfjoch_viewer: Major redesign with dockable panels and saved layouts, plus on-canvas creation/move/resize of box, circle and azimuthal ROIs * jfjoch_viewer: Run jfjoch_process reprocessing jobs from inside the GUI and overlay per-run results Reviewed-on: #63	2026-06-23 20:29:49 +02:00
leonarski_f	cc3eb8352c	v1.0.0-rc.148 (#58) ... This is an UNSTABLE release. The release has significant modifications for data processing - in case of troubles go back to 1.0.0-rc.144. * jfjoch_broker: Improve azimuthal integration (add <I^2> calculation) * jfjoch_broker: Fixes around indexing, aiming to handle multi-lattice crystals (work in progress, it is not fully integrated) * jfjoch_writer: Save mean(I), stddev(I), and count(I) for each azimuthal bin Reviewed-on: #58	2026-06-08 08:30:35 +02:00
leonarski_f	239a441ee6	v1.0.0-rc.140 (#50) ... This is an UNSTABLE release. The release has significant modifications and bug fixes, if things go wrong, it is better to revert to 1.0.0-rc.132. * jfjoch_broker: For DECTRIS detectors, ZeroMQ link is persistent, to save time for establishing new connection * jfjoch_broker: Minor bug fixes for rare conditions Reviewed-on: #50	2026-04-29 21:40:22 +02:00
leonarski_f	c1c170112c	v1.0.0-rc.136 (#45) ... This is an UNSTABLE release. The release has significant modifications and bug fixes, if things go wrong, it is better to revert to 1.0.0-rc.132. * jfjoch_broker: Improve logic regarding indexing architecture and thread pools (work in progress). Reviewed-on: #45	2026-04-20 11:54:33 +02:00
leonarski_f	6133da1377	v1.0.0-rc.133 ... This is an UNSTABLE release. The release has significant modifications and bug fixes, if things go wrong, it is better to revert to 1.0.0-rc.132. * jfjoch_broker: Use httplib for HTTP server instead of Pistache * jfjoch_broker: Drop OpenSSL support * jfjoch_broker: Base work for multi-lattice support in the future * Update dependencies to more recent versions (spdlog, HDF5, Catch2, httplib) Reviewed-on: #41	2026-03-26 20:50:33 +01:00
leonarski_f	27496b8207	v1.0.0-rc.122 (#29) ... This is an UNSTABLE release. * jfjoch_broker: Add thresholding to prefer shorter vectors after FFT * jfjoch_broker: Add experimental mosaicity estimation for rotation experiments (this is work in progress) * jfjoch_viewer: Display file opening errors * jfjoch_viewer: When loading files over DBus add retry/back-off till the file is available Reviewed-on: #29 Co-authored-by: Filip Leonarski <filip.leonarski@psi.ch> Co-committed-by: Filip Leonarski <filip.leonarski@psi.ch>	2025-12-16 15:27:40 +01:00
leonarski_f	06949caf1a	v1.0.0-rc.112 (#18) ... This is an UNSTABLE release and not recommended for production use (please use rc.11 instead). * jfjoch_broker: Experimental rotation (3D) indexing * jfjoch_broker: Minor fix to error in optimizer potentially returning NaN values Reviewed-on: #18 Co-authored-by: Filip Leonarski <filip.leonarski@psi.ch> Co-committed-by: Filip Leonarski <filip.leonarski@psi.ch>	2025-11-30 17:39:22 +01:00
leonarski_f	f44c6520a8	v1.0.0-rc.107 (#12) ... This is an UNSTABLE release. * jfjoch_viewer: Minor polishing of new functionality * jfjoch_broker: User NaN for empty azimuthal bins Reviewed-on: #12 Co-authored-by: Filip Leonarski <filip.leonarski@psi.ch> Co-committed-by: Filip Leonarski <filip.leonarski@psi.ch>	2025-11-24 07:07:32 +01:00
leonarski_f	b2abb0f92b	v1.0.0-rc.94	2025-10-25 22:05:47 +02:00
leonarski_f	5d9d2de4a4	v1.0.0-rc.81	2025-09-21 19:27:51 +02:00
leonarski_f	20973792e4	v1.0.0-rc.68	2025-08-16 19:59:27 +02:00
leonarski_f	41a3e671f4	v1.0.0-rc.41	2025-06-10 18:14:04 +02:00
leonarski_f	53c90ee5d8	v1.0.0-rc.40	2025-05-28 18:49:27 +02:00