15 Commits

Include renames

Author	SHA1	Message	Date
leonarski_fandClaude Opus 5.5	0cf62452cd	Stills: kept overloads go back to the drop where they are not concentrated at low resolution ... Saturation clips the strongest spots, and those are at low resolution. On a Rayonix stills set the saturated pixels sat almost entirely past 4 A (0.002% of the reflections coarser than 4 A against 0.59% overall) - flagged or hot pixels, not clipped spots - and keeping those observations as lower bounds put the saturation limit into high-resolution intensities: R_split 0.12 -> 0.93, CC1/2 0.99 -> 0.33. The run now keeps overloads only where their share coarser than 4 A is at least 1.5x their overall share; otherwise they are flagged and dropped as before, with a log line saying so. On clipped CCD stills the share coarser than 4 A is 2.6-5.9x the overall one and nothing changes (R_split and R_free identical); on the Rayonix set R_split returns to 0.12. A pragmatic gate until saturation is told from bad pixels per spot. Rotation never keeps overloads and is unaffected. Co-Authored-By: Claude Opus 5.5 <noreply@anthropic.com> Claude-Session: https://claude.ai/code/session_015CeEGgpKdfkCTJb3YNMJcu	2026-10-22 13:51:47 +02:00
leonarski_fandClaude Opus 5.5	6b5647e8ab	Merge stills-sat into stills-easy ... The one conflict, tests/BraggIntegrationEngineCPUTest.cpp, where both branches add cases at the same place: integ-pal's side is taken and stills-sat's test diff applied on top, which keeps all four cases. Co-Authored-By: Claude Opus 5.5 <noreply@anthropic.com> Claude-Session: https://claude.ai/code/session_015CeEGgpKdfkCTJb3YNMJcu	2026-10-22 12:46:00 +02:00
leonarski_fandClaude Opus 5.5	72cc542d78	Stills keep an overloaded observation as a lower bound instead of dropping it ... The stills merge dropped every observation with a saturated pixel. On a still the saturated observations are the fully recorded ones of the strongest low-resolution reflections, so what survived were their partial observations, whose partiality correction then set the merged intensity: on clipped CCD stills the merged low-resolution intensities came out at 0.4-0.6x of the deposited ones, a ramp no Wilson B absorbs, invisible to CC1/2 and R_split. The pixels are really clipped (flat-topped plateaus a few per mille wide, a pile-up in the pixel-value histogram from the per-pixel ADC limit), so the auto ceiling is right; the drop was the defect. A still now keeps the observation: the box sum with every saturated pixel counted at the saturation limit, unflagged and marked clipped, counted in BraggIntegrationCounts and reported as OVERLOADED_REFLECTIONS_KEPT. Rotation data (IsRotationIndexing) are unchanged and keep the flag for the rocking-event drop. Measured on a clipped-CCD stills subset (dimple R-free, deposited free set): dropped 0.247, lower bound 0.230 (same as switching saturation off). A Kabsch fit to the unsaturated wings read lower than the lower bound (0.237), and inflating the lower bound's sigma lost (0.255). Co-Authored-By: Claude Opus 5.5 <noreply@anthropic.com>	2026-10-22 10:36:33 +02:00
leonarski_fandClaude Opus 5.5	07a43a13eb	Stills: the radial curvature correction decided per run on the same empty apertures ... The first stills battery of e8145d8 lost on one Rayonix set (lcls242_s, dimple R_free 0.2302 -> 0.2323): there the whole-frame radial correction hurts. On 40,000 of its frames: battery default 0.2462, ring 12 with the correction 0.2444, ring 12 without it 0.2336, ring 14 with it 0.2467. Its beam is strongly polarised and the azimuthally averaged ring background does not describe the local background. So the empty apertures now also carry the corrected difference: the frame's ring background (RingBackground, factored out of the engine) averaged over the ring pixels minus over the disk pixels - what the integrator's kernel takes off a reflection - is subtracted from each disk-minus-ring difference. The ring is still chosen on the plain differences, so its reach does not rest on the radial model; where the correction was left to auto it is then kept only if it makes that ring predict the disk better. Decisions on 15-60 pre-scan frames: pal86 ring 10, correction on (240.6 -> 221.1) lcls222 ring 10, on (6.34e4 -> 3.41e4) lcls242_s ring 12, off (277.2 -> 285.8) alvra213_int16 ring 14, on (0.01424 -> 0.01422) Choosing ring and correction jointly instead picked ring 14 with the correction on lcls222, where dimple reads 0.204 against 0.196 at ring 10; a median instead of the mean square picked ring 14 with the correction on lcls242_s, the worst arm there. The sequential rule is the one that agrees with dimple on every set measured. Co-Authored-By: Claude Opus 5.5 <noreply@anthropic.com> Claude-Session: https://claude.ai/code/session_015CeEGgpKdfkCTJb3YNMJcu	2026-10-21 20:58:32 +02:00
leonarski_fandClaude Opus 5.5	e8145d8d2f	Stills integration: background ring reach measured on empty apertures, radial curvature from the whole frame ... Two changes to the stills integration background, both stills-only (rotation keeps its path bit for bit): 1. The r2..r3 background ring's outer radius is measured per run. The pre-scan lays apertures on a grid over its frames, away from every found spot, and for each candidate r3 (r2+2 .. 14) takes the mean square difference between the r1 disk mean and the clipped ring mean. With nothing in the aperture that is exactly the background error the ring makes (noise + bias); the run keeps the minimum. On a photon-counting pixel detector the noise wins and the shipped r3=14 is kept; on a binned CCD the background structure wins and the narrowest ring is taken. r1 stays 6: a smaller disk (4,6,14) costs 0.0013 dimple R_free on a JUNGFRAU set, so it does not pass the photon-counting gate. --adaptive-integration-radius now defaults on for stills too (=off restores the fixed 6/8/14). The pre-scan bandwidth estimate is not applied to stills. 2. The radial background-curvature correction on stills takes its curve from the adaptive spot finder's peak-excluded per-ring background (whole frame) instead of the predicted reflections' own ring pixels, and auto applies it to every stills image (no ice-score gate: a solvent/carrier hump curves the background as much as ice). New engine call RadialBackgroundFromRings; CPU, GPU and Metal read the handed-over curve. The GPU box sum now sizes the radial bin index separately from accumulating, so a handed-over curve is read at the right radius. Measured (dimple R_free, deposited free set, battery arguments, all frames unless noted): pal86 (Rayonix 4x4, 156 um): 0.354 -> 0.218 (ring 10; at 4,6,10 0.213) lcls222 (Rayonix 4x4, 177 um): 0.205 -> 0.196 (ring 10) sacla236 (MPCCD): 0.2588 -> 0.2558 (ring 11) alvra213_int16 (JUNGFRAU): 0.1986 -> 0.1986 (ring 14, unchanged) Co-Authored-By: Claude Opus 5.5 <noreply@anthropic.com> Claude-Session: https://claude.ai/code/session_015CeEGgpKdfkCTJb3YNMJcu	2026-10-21 18:10:08 +02:00
leonarski_fandClaude Opus 5.5	d6166f6fa5	Panel layout stage 2: prediction and Bragg integration through the panel table ... Everything sparse that took a radial quantity from an image coordinate now takes it from the reflection's (or spot's) position on the detector plane, through its panel (DetectorModules). With an empty module table every changed expression reduces to the old one in the same floating-point order, so flat detectors - every rotation set, EIGER, CCDs, assembled JUNGFRAU - integrate bit for bit as before. - Prediction (CPU, GPU, rotation CPU and GPU): bounds test against PlaneBounds instead of the image rectangle. - IntegrateOnImage: a prediction in a gap or off every panel is dropped (PlaneToPanel), no longer passed through onto an unrelated stored pixel. The panel id stays local: the engine and the way back find it from the image position (the panel boxes tile the image), and a prediction that rounding to float put on another panel's edge is dropped so the two agree. Nothing is added to Reflection. - Bragg engines (CPU, CUDA, Metal) take a BraggPanel per reflection (BraggStencil.h): its plane position, the panel's pixel axes on the plane and its box. The stencil's radial direction is taken on the plane and expressed in the panel's pixel axes; r0, the radial background curve, the Gaussian's elongation, the learned moments, tan(2theta) and Finalize's polarisation use the plane position; r_max / n_rad come from PlaneBounds. The neighbour mask and the owner map are clamped to the reflection's own panel; inside the walked box a pixel off the reflection's panel is read as a gap (unreadable, statically masked - not an overload), which is what the assembled image has there, so a disk cut by a panel edge is partial rather than silently "full". - Risk R4: the ProfileEmpirical grid is learned and applied in the plane's axes (the panel axes taken to the nearest quarter turn, BraggProfileCell), so turned panels pool one shape. Without it the stacked layout read up to 0.3 % off the assembled one in the harness. - SpotWidth / SpotFootprint: aperture bounds against the spot's panel box, beam distance, resolution and the shape's 2theta Jacobian on the plane, moments read in the panel's axes. - GetDetectorMaxQ_recipA, the far-corner radii (first-pass tilt report, metric-symmetry arm, footprint table range) from PlaneBounds; pre-scan spot resolution on the plane; LogHeaderBeamCenter: geometric centre of the panels' plane box, and the masked-pixel check on the panel the beam lands on (none when it is in a gap). Harness: PanelLayout_BraggIntegration is now a real [PanelLayout] check, over six settings (default, bandwidth-elongated ring, radial background, overlap exclude, box sum, empirical profile, all with polarisation), stacked vs assembled to 1e-5; PanelLayout_BraggIntegrationGPU runs the same on the CUDA engine. Its spots avoid exact half pixels: the grid centres on the rounded position, and a half rounds to the other neighbour on a turned panel. The Metal engine (.metal/.mm) mirrors the CPU change exactly but is UNCOMPILED here (no macOS): it needs a build and BraggIntegrationEngineMetal_BitIdenticalToCPU on a Mac. Co-Authored-By: Claude Opus 5.5 <noreply@anthropic.com> Claude-Session: https://claude.ai/code/session_015CeEGgpKdfkCTJb3YNMJcu	2026-10-21 10:40:20 +02:00
leonarski_fandFilip Leonarski	19b135186d	v1.0.0-rc.175 (#85) ... * Rugnux: Processes a collection live while jfjoch_broker writes it (`rugnux <master.h5> <broker URL>`). * Rugnux: Processing starts on the first images and confirms its choices once all are in, so analysis can begin during collection. * Rugnux: Faster processing, especially on servers with several GPUs and CPU sockets and on computers without a GPU (`--no-gpu`, macOS). * Rugnux: Uses much less GPU memory, so large data sets stay on the GPU of smaller cards, and a data set too large for the card is processed on the CPU instead. * Rugnux: On macOS, Bragg integration runs on the Apple GPU. * Rugnux: Better handling of twinning and pseudo-symmetry, with the twin hypothesis written as `<prefix>_twin_<SG>.mtz`, and a wrong `--model` no longer confirms the data or decides the hand. * Rugnux: `--model` accepts predicted (AlphaFold) models and falls back to molecular replacement when the model is not placed as a rigid body (experimental `--mr` forces it), settling space group, hand and twinning and writing a different answer as `<prefix>_mr.mtz`. * Rugnux: Molecular replacement is faster and settles the space group in more cases with several copies in the asymmetric unit. * Rugnux: Deposition-ready mmCIF, a richer report, and numbered steps on the terminal with the full log in `<prefix>_log.txt`; `_P1.mtz`, `--estimate-beam-center` and `--beam-center-search` are removed. * Rugnux: The beam-stop shadow is found correctly on tilted detectors. * Rugnux: Stills files that record a stationary goniometer axis get the default stills geometry refinement. * jfjoch_viewer: "Analyze dataset" uses the same defaults as a bare `rugnux <file>`, and shows the results of processed CBF, marCCD and SMV sweeps. * jfjoch_viewer: The Files panel refreshes on F5 and every few seconds, and the plot type and other selections stay put during live collection. * jfjoch_writer: Memory stays bounded and old data files are closed efficiently on long runs, any failure ends the run in an error state the broker is told about, and the master file appears only after its data files; the ZeroMQ pusher logs when a stalled writer makes it drop images. * Fixes: The TCP image pusher no longer blocks the broker's receiver, GPU out-of-memory failures stop with a clear message, and the XDS plugin masks module and chip edges. --------- Co-authored-by: Filip Leonarski <jungfrau@filips-mac-mini.home> Reviewed-on: #85 Co-authored-by: Filip Leonarski <filip.leonarski@psi.ch>	2026-10-16 15:34:43 +02:00
leonarski_f	a395f358ef	1.0.0-rc.174 (#84) ... * Rugnux: Performance improvements on GPU and CPU (more of the pre-scan and of scaling on the GPU, faster CPU spot finding and crystal refinement), with unchanged results. * Rugnux: More robust processing - patches of persistently hot pixels are masked, an inconsistent merge triggers a retry at the measured beam centre, and builds targeting different CPU levels give the same results. * Rugnux: Improved scaling and merging - reflections with an overloaded pixel are dropped, as in XDS, sparse rotation sweeps are scaled more reliably, and French-Wilson amplitudes use an anisotropic Wilson prior. * Rugnux: Improved space-group determination - glide planes in groups without a centre of symmetry, screw axes from short or weak axial rows kept when a higher group is adopted, and more reliable decisions on twinned and pseudo-symmetric crystals. * Rugnux: Improved small-molecule processing - spots that grow wider than the integration disk and split spots are integrated over their measured footprint, sparse lattices are integrated on every frame, and the `.hkl` file holds unmerged scaled reflections (SHELX HKLF 4). * Rugnux: Reads Rigaku d*TREK SMV images (Saturn CCD), including detector 2theta and encoded pixel overflows; home-source (rotating-anode) datasets were added to the validation battery. * jfjoch_viewer: Fixed processing failing at the end with "Wrong JPEG library version" on Linux; the merge window shows the space group with proper subscripts and a checklist of crystal pathologies. Reviewed-on: #84 Co-authored-by: Filip Leonarski <filip.leonarski@psi.ch>	2026-10-06 14:03:18 +02:00
leonarski_f	84228bf8be	v1.0.0-rc.173 (#83) ... * jfjoch_broker: Optional per-dataset authentication - statistics, images and plots can require a bearer token, which jfjoch_viewer supports. * jfjoch_viewer: Dark mode and a theme-matched colour scheme, a magnifier panel, and simpler contrast and background controls. * Rugnux: Multiple performance improvements on GPU and CPU (CPU-only processing up to 40% faster, faster image decoding on ARM), with unchanged results. * Rugnux: `--model` rigid-body refinement runs on the GPU, and the model-validation check is faster and more reliable. * Rugnux: Improved scaling and merging - error model, outlier rejection, absorption correction and French-Wilson amplitudes now agree more closely with XDS and ctruncate. * Rugnux: Improved integration - radial background on powder and ice rings, crowded rotation data keep their reflections, and CPU-only builds integrate large unit cells as GPU builds do. * Rugnux: More robust detector geometry - measured beam centre, X-ray bandwidth and goniometer rate, and geometry refinement accepted only on significant evidence. * Rugnux: Merged files are written in the standard setting, or in the setting of a reference MTZ, structure-factor mmCIF or model, with its free-R flags. * Rugnux: Richer report - ice and powder rings, further lattices, superstructure candidates and mosaicity, with warnings worded as prompts to check. * Rugnux: Clear error messages when a data set needs more GPU or host memory than is available. Reviewed-on: #83 Co-authored-by: Filip Leonarski <filip.leonarski@psi.ch>	2026-09-29 15:57:32 +02:00
leonarski_f	6dfe065365	v1.0.0-rc.172 (#82) ... * Fixed `jfjoch_broker` cancelling every data collection with a CUDA "out of memory" error after long operation: GPU memory no longer leaks with each collection. * Rugnux scales a rotation sweep until the per-frame scales settle instead of for a fixed three rounds, and says so when they did not - merged intensities, and the space group, resolution cut and frame rejection read off them, change accordingly; `--scaling-iterations` is now the cap on that loop (default 100). * Rugnux places every frame of a marCCD, SMV or miniCBF series at the spindle angle its own header states, so a series with missing frames, or with angles written modulo 360, is no longer read at the wrong geometry or refused. * Every rotation run writes two diagnostic files beside its reflections: `<prefix>_detector.jpg`, the detector projection with the pixel mask and the detected beam-stop shadow drawn on it, and `<prefix>_plot.txt`, one row per image. Reviewed-on: #82 Co-authored-by: Filip Leonarski <filip.leonarski@psi.ch>	2026-09-22 06:48:37 +02:00
leonarski_f	a39fd29f77	v1.0.0-rc.167 (#77) ... * `rugnux --model` reports CC(model, data) - the correlation of the merged intensities with the placed, scaled model - by resolution shell, on the same shells as CC1/2, with the reflection count and a significance for each. * `rugnux --model` fits the model's scale, anisotropic B and bulk-solvent parameters on the working reflections only, so the R-free it reports is measured against a model no free reflection helped scale. * The bulk-solvent parameters of `rugnux --model` are searched over their physically meaningful range instead of being fitted without bounds, so a model is never scaled with a solvent term that has silently switched itself off. * The rigid-body placement of `rugnux --model` uses the same bounded bulk solvent as the reported fit, so a model is no longer placed against a target carrying a solvent term with no physical meaning. * `rugnux --model` puts the model into the data's own description of the lattice before placing it, so a model whose cell is written on other axes - I-centred where the run indexed C-centred, a different unique axis, a permuted orthorhombic cell - is placed rather than scored where it was read; `MODEL_CHANGE_OF_BASIS=` and `MODEL_SETTING_AS_READ=` report it when it happens. * The rugnux results report opens with a summary - `VERDICT=` (`OK`, `WARNINGS`, `UNUSABLE`, `FAILED`), `VERDICT_TEXT=`, `PATHOLOGY_FLAGS=` with one closed-vocabulary code per condition that warned, and the `WARNING:` lines, which used to close the file - and the sections after it are renumbered 1-5 with no gaps. * `rugnux --developer` writes the full results report - the pipeline-internal keys and the long explanations the default report now leaves out - and `--finalist-ledger` adds the evidence for every space group the search considered, not only the one it adopted. * The results report warns when the merged data carry no usable signal and when too little of reciprocal space was measured inside the fitted resolution, and omits `FITTED_RESOLUTION` where the CC1/2 curve it is fitted on never falls off. * rugnux detects translational pseudo-symmetry and reports it under the `PSEUDO_TRANSLATION` flag as `TNCS_DETECTED=` and the `TNCS_*` keys - a translation the merged data are exactly invariant under is reported as `UNDECLARED_LATTICE_TRANSLATION=` under `LATTICE_TRANSLATION` instead - and a detected pseudo-translation can no longer buy a false screw axis in the space-group search or hide a twin from the L-test (`L_TEST_VS_TNCS=`). * The space-group search determines glide planes from zonal systematic absences, so a non-Sohncke space group such as P 2_1/c or Pbca is named where the run previously stopped at its Sohncke subgroup; `SOHNCKE_SPACE_GROUP=` carries the best Sohncke group beside it on every run that searched, and a centre of symmetry is never claimed. * Where the cell metric carries more rotational symmetry than the Bravais class the indexer named, the extra rotations are put to the intensities and the space-group search is asked again on the metric's own cell - adopted only where the intensities confirm the higher symmetry - so a lattice that is nearly but not exactly hexagonal, or whose reduction landed in a sub-cell, still reaches its true point group. * Systematic-absence calls rest on the evidence rather than on counts: a screw axis whose absent class the data show extinct is no longer refused because a handful of reflections in it read as present, and `SPACE_GROUP_ALTERNATIVES=` no longer drops a candidate that differs only on a zone the sweep never measured. * A reference correlation measured on too few reflections is refused instead of scored zero, so a run given a reference MTZ is no longer reindexed on an operator that mapped almost everything outside the reference's coverage. * A frame counts as indexed from 6 spots on its lattice rather than 9, so a weakly diffracting crystal whose frames cannot carry 9 is no longer refused the lattice it fits; `--min-indexed-spots` overrides it. * `-C` accepts a known cell in any equivalent description - conventional or primitive, centred or not - instead of only the reduced primitive form, so a centred cell given the way it is published no longer makes the run report that it found no lattice. * Each reflection is corrected for the sensor's quantum efficiency at the angle it meets the detector (attenuation lengths from the NIST tables, which also fixes the spot-width parallax term on CdTe) and for the attenuation of the flight path between the sample and its pixel; `--flight-path air|helium|vacuum` declares the medium - default air, since no file states it - and the report says what was assumed and what it was worth. The unmerged MTZ records the factors in new `QE` and `FLIGHT` columns beside `LP`, so raw counts are `I / LP * QE * FLIGHT`, and `_process.h5` in new optional `qe` and `flight` datasets. * Rotation geometry post-refinement fits the crystal and the detector at once, against the observed spot positions and the observed rocking angles together, so the refined distance depends far less on how wrong the file's distance was. * A coarsely sliced sweep integrates correctly: partials are joined into one rocking event by angle rather than by frame count, so two crossings of the Ewald sphere are no longer summed into one full, and at 0.5 degrees per image or coarser the per-frame geometry refinement accepts a spot whose miss the exposure's own rotation accounts for. * `rugnux --mode scale` reports the detector tilt and direct beam of the geometry it re-scaled at, instead of zeros that read as a flat detector, and no longer warns that no image was indexed on a run whose lattice came from its input file. * Every rotation run that determined a space group and merged reports what the mounting cost: `SPINDLE_LOST_UNIQUE_FRACTION=` is the fraction (0-1) of unique reflections the mounting made unmeasurable under the measured point group, also written to the master as `/entry/MX/spindleLostUniqueFraction` and what the mounting warning fires on; `SPINDLE_SYMMETRY_AXIS_ANGLE_DEG=` / `SPINDLE_SYMMETRY_AXIS_ORDER=` describe the mounting in the `--developer` report. * Stills and grid scans carry a per-image `spindle_blind_fraction` - how much of a rotation sweep's blind cone this orientation would make unrecoverable, 0.5 and above calling for a second orientation - through the CBOR stream, HDF5 (`/entry/MX/spindleBlindFraction`), the plot and scan-result APIs, and the viewer and frontend plots; an absent value means the frame could not be assessed and is not a 0. * The results report's `REPORT_VERSION` is 7. Reviewed-on: #77 Co-authored-by: Filip Leonarski <filip.leonarski@psi.ch>	2026-09-09 07:25:13 +02:00
leonarski_fandjungfrau	4dc2534dbf	v1.0.0.rc-162 (#72) ... **Files written by Jungfraujoch now import correctly in DIALS, XDS and pyFAI.** A tilted detector, a grid scan, a still recorded at a goniometer position, and saturated or unreadable pixels were each described in a way that a third-party program acted on wrongly. If you process Jungfraujoch data outside Jungfraujoch, prefer this release to any earlier one. * HDF5: the detector tilt (`rot1`/`rot2`/`rot3`) is exported correctly in the NXmx transformation chain; untilted geometries are unaffected. * HDF5: a still recorded at a goniometer position is no longer read back as a single image, and a grid scan records a stationary spindle so a program that requires a rotation axis can open it. * HDF5: the sample transformation chain is written in mounting order, with a Smargon head position told apart from the spindle, one entry per image, `module_offset` as a float unit vector, and `offset_units` on every offset. * HDF5: saturated, underloaded and unreadable pixels are described so a downstream program masks them - `saturation_value`, `underload_value`, `error_value` and `bit_depth_readout` are written correctly, and a data file missing next to a VDS master reads as the error marker rather than as zero counts. * HDF5: the rotation axis is read back under whatever name it carries, and `mirror_y` records whether the assembled image is mirrored in Y relative to the detector's raw readout. * A grid scan and a goniometer axis can both be set; they are no longer alternatives. * `images_per_file` is chosen from the acquisition when it is not given: a rotation sweep of at most 20000 images goes into a single data file, a grid scan splits on whole fast-axis rows, and stills and serial keep 1000. * The writer refuses a stream whose start message declares a different pixel format than its images carry, and a DECTRIS detector sending signed images is no longer declared unsigned. * The image stream can carry the sample transformation chain (`transformations`, in the END message); a producer that does not send it gets the same chain built by the writer. * rugnux: fixing the space group with `-S` no longer prevents the lattice from being found - a lattice indexed in a different setting is reindexed into that group's own setting, and a run whose crystal does not have that group's lattice stops and names the cell it indexed as, rather than reporting statistics that cannot describe it. * rugnux: the per-image resolution estimate now predicts the resolution the merged data reach rather than the highest-resolution spot found, and is reported as `SPOT_RESOLUTION_ESTIMATE`. * rugnux: two runs of the same command on the same images produce the same merged intensities; the azimuthal profile written alongside them is not yet reproducible in the same way. * rugnux: the offline lattice refinement is bounded by iterations rather than by a wall clock, so a loaded machine can no longer refine to a different lattice; a live acquisition keeps its real-time bound. * rugnux: the detector-frame modulation correction is fitted on a grid spanning the detector, so whether it is applied no longer depends on how far integration reached. * rugnux: the geometry pre-pass no longer writes `<prefix>_01.mtz`, `_01.cif`, `_01.hkl` and `_01_image.dat`; the refined second pass writes those files under `<prefix>`, and that is the result to use. * rugnux: `_process.h5` describes the pixel format of the images it links to, and is written on a thread of its own. * rugnux: the detector geometry is also logged in XDS's convention (`ORGX`/`ORGY`, detector axis vectors, rotation axis), so it can be compared with an XDS refinement. * rugnux: an image integrated in pyFAI through the `.poni` file written by `--mode calibration` comes out with the correct azimuth, and the file declares pyFAI's `orientation`, which needs pyFAI 2024.01 or newer. Radial integration is unchanged. * rugnux: a rotation run is substantially faster throughout - beam-stop detection, first-pass indexing, geometry refinement, integration, scaling and merging - and observations outside the scaling resolution range are dropped as they are ingested. The refined geometry, the space group chosen and the merged statistics are unchanged. * Faster spot finding and indexing, on the broker as well as in rugnux; the spots found and the lattices indexed are unchanged. * A run reserves substantially less GPU memory: nothing is allocated for buffers that are never read, and a worker builds only the engines it uses. * rugnux: with `-N` left at its default the per-image loop of `--mode mx` uses at most 16 workers per GPU, rather than one per hardware thread; an explicit `-N` is obeyed as given. * CUDA 12 builds now contain device code for Volta, so the RHEL 8 packages and the portable Linux `.tgz` run on a V100; the CUDA 13 artefacts (RHEL 9, Ubuntu, Windows) remain Turing and newer. * The build resolves a single Eigen for the whole project, and refuses to configure if Ceres picks up a different one; a build that mixed two Eigen versions was undefined behaviour and crashed at -O2. * Documentation: a security page, and the supported GPU generations and minimum NVIDIA driver version of every released artefact. **Breaking change to OpenAPI** - regenerate the client (`jfjoch-client` 1.0.0-rc.162, `frontend/src/client`): * `dataset_settings.images_per_file` is no longer `default: 1000` and no longer accepts `0`; it is optional, and its minimum is 1. A client sending `0` (previously "one file for the whole run") is now rejected - omit the field instead, which for a rotation sweep gives the same single file. * `file_writer_format` now defaults to `NXmxVDS`, matching the server's own default and the layout recommended for DIALS, XDS and CrystFEL. A generated client that fills in schema defaults and does not set the format explicitly will write VDS masters where it previously wrote legacy ones; set `NXmxLegacy` explicitly to keep them. --------- Co-authored-by: jungfrau <jungfrau@mx-aare-test.psi.ch> Reviewed-on: #72 Co-authored-by: Filip Leonarski <filip.leonarski@psi.ch>	2026-08-25 08:21:39 +02:00
leonarski_f	538f3504d3	v1.0.0.rc-161 (#71) ... 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: significantly better quality of results, and faster.** A large rework of integration, scaling, merging, geometry refinement and space-group determination, together with measurements the program previously made no attempt at - the direct beam before indexing, the beam stop, the goniometer rotation scale, and the stretches of a sweep the crystal did not deliver. A rotation dataset typically gains observations at better <I/sigma> and R_meas, and every `mx` and `scale` run writes a `<prefix>_report.txt` results report modelled on XDS's `CORRECT.LP`. Many defaults moved with it: spot detection is self-calibrating, beam-stop detection and rotation geometry post-refinement are on, resolution limits default to as far as the detector reaches, and ice-ring handling engages only where the crystal is measured to have ice. * **jfjoch_viewer:** the beam-stop shadow, the detector calibration and the beam-centre measurement are reachable from "Analyze dataset"; the settings panel reports how the sample moved and how polarized the beam was; image rendering and interaction are faster. * **Performance:** bitshuffle+LZ4 images are decoded on the GPU rather than on the host, with the bitshuffle inverse fused into preprocessing so the decompressed frame is never held in device memory. * **Broker, writer, packaging and build:** image-slot lifetime and locking fixes, per-image datasets sized by the images actually written, the Debian/Ubuntu broker package renamed to `jfjoch`, and `image_analysis` compiling under MSVC again. **Breaking change to the rugnux command line:** * `--azint-only` and `--scale` are **removed**, replaced by `--mode azint` and `--mode scale`; the full pipeline is `--mode mx` and remains the default. A script passing the old flags now fails with the list of valid modes rather than silently running the wrong one. * `-t`/`--stride` is **refused on rotation data**: skipping frames cuts every reflection's rocking curve, so the combined fulls and their partiality would be measured over frames the sweep never recorded. Select a contiguous range with `-s`/`-e` instead. `--mode azint` and `--force-still` still take a stride. **Breaking changes to OpenAPI** - regenerate the client (`jfjoch-client` 1.0.0-rc.161, `frontend/src/client`) or read the affected fields as optional: * `image_scale_b` is removed from the `plot_type` enum, so a client requesting that plot now gets an error rather than a curve. * `azim_int_settings.high_q_recipA`, `spot_finding_settings.high_resolution_limit` and `spot_finding_settings.low_resolution_limit` are no longer `required`. All three mean "no limit at that end" when unset and are omitted from the response instead of carrying a placeholder value, which raises in a client generated from an rc.160-or-earlier spec. A value of 0 is still accepted and means the same thing. **Breaking changes to the stored formats** - a consumer reading these fields must treat them as optional: * The per-image image-scale B factor is no longer computed, so `/entry/MX/imageScaleBFactor` is absent from newly written HDF5 files and the corresponding key is absent from the CBOR DataMessage and END blocks. Files written by rc.160 and earlier still contain it and still open; nothing in the pipeline reads it any more. * `_reflns.jfjoch_diffrn_ISa` now carries the whole-range `1/sqrt(a*b)` that XDS's ISa denotes, and the error-model `a` and `b` are reported in XDS's convention; the strong-reflection asymptote moves to `_reflns.jfjoch_diffrn_ISa_asymptotic`. **A file written by an earlier version carries the asymptote under the plain `ISa` name.** Reviewed-on: #71 Co-authored-by: Filip Leonarski <filip.leonarski@psi.ch>	2026-08-13 17:03:10 +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