12 Commits

Include renames

Author	SHA1	Message	Date
leonarski_fandClaude Fable 5.1	40874c2c2d	Space-group search: the twin-immune zone is read on a normalisation the control certifies ... The zone verdict that arbitrates a refused promotion read its zone absolutely, against the centric and acentric Wilson expectations, and an absolute reading is only as good as the normalisation under it. On two refused 622 promotions - a 6/m crystal and a 312 one, whose added operators disagreed at 4.7x and 5.2x the parent's H and merged to an R_meas of 0.34 under the higher group - every class read centric: a 67 A^2 anisotropy, isotropically normalised in bins of 100, spread one shell's expected intensity over a factor of 15 between its directions, and the acentric control read 1.00 against its 0.74. The zone read the same as the control, +0.10 nats per reflection, and +124 nats over 947 reflections rescued a twin law. Two things change. The anisotropy is fitted on the acentric reflections of the shells read (ln I = c + s^T Q s, by least squares) and its deviatoric part taken out of every intensity before anything is normalised; that alone brings the controls of the crystals measured to 0.73-0.77. What no normalisation removes, the control then certifies: an acentric population reads -0.130 nats per reflection when the normalisation is right, a twinned one reads below that, so whatever the control reads above it is the normalisation's - anisotropy, a pseudo-translation, a pseudo-centring, noise all inflate every class towards centric alike - and the zone, normalised the same way, carries the same per reflection; the calibrated evidence has it taken off, and that is what the verdict reads. The two rescued twin laws now read -130 and -78 nats and stay refused, with the law named; the genuine promotions measured read +137 to +580 (a pseudo-centred orthorhombic crystal whose control reads 0.99 still +334); the trigonal and hexagonal partial twins -129 to -420 as before. The report prints the control's excess and the calibrated evidence beside the raw one. The metric-lattice re-ask carried a second copy of the two-arm rule without the zone: a P31 partial twin whose 32 the main rule had refused on the zone was promoted by that ask's Lorentz-filtered arm. It now puts the same verdict to a refusal the other arm would outvote. Co-Authored-By: Claude Fable 5.1 <noreply@anthropic.com> Claude-Session: https://claude.ai/code/session_013nW6FNRP1bBJJ8pfHiByAT	2026-09-20 18:45:17 +02:00
leonarski_fandClaude Fable 5.1	004839a8ee	Space-group search: the twin-immune zone arbitrates a refused promotion ... A promotion the operator correlations confirm and a gate refuses (the H ratio, the added-operator R, the merge chi^2) used to be settled two ways that both read the per-frame scales: the two-arm rule let the other arm's confirmation outvote the refusal, and the remerge arbiter compared the R_meas and ISa of the two pinned merges. Neither holds once the scales have settled: a partial twin at a fraction one arm's coverage hides passes there (an H3 twin promoted to R32, a P31 one to P3121), and the lower group's converged merge - the same scales fitted against fewer equivalents - agrees with itself better than the true group on a genuine step (a 2 -> 222 step reading R_meas 0.094 -> 0.103), so the arbiter refuses real symmetry. The refusal is now decided by the twin-immune zone of the operators the promotion adds: the reflections centric in the higher group and acentric in the lower are their own twin mates, so they read centric if the operators are real and acentric if they are a twin law or a pseudo-symmetry, whatever the twin fraction and however the scales were fitted. Read on the all-observation P1 merge in the two-arm rule and on the adopted group's own merge at the arbiter (where a weak crystal's P1 search merge has no shell with signal to read), for a group two orders above the other, with the pseudo-translation normalisation the L-test uses, and decided on the sign with the screw-axis convention of 20 nats: acentric and the refusal stands on all observations, centric and the higher group is adopted, undecided and the rules stay as they were. Measured: a genuine 222 step reads +150 to +1630 nats, the trigonal twins -130 nats and below. A refusal that stood on the zone names the law: the first operator the refused group adds, at the fraction the operator's own H implies (else the pre-search L-test), reported as TWIN_LAW and written as the mmCIF _pdbx_reflns_twin loop of the merge in the true group. Every lattice twin law outside the adopted group is reported with its own H, implied fraction, R and correlation on the merge expanded to P1 (TWIN_LAW_n), following Yeates (1997) Methods Enzymol. 276, 344-358. Co-Authored-By: Claude Fable 5.1 <noreply@anthropic.com> Claude-Session: https://claude.ai/code/session_013nW6FNRP1bBJJ8pfHiByAT	2026-09-20 18:45:17 +02:00
leonarski_fandClaude Opus 5	3d62388467	Twin-immune zone evidence for the operators a promotion adds (report-only) ... Under a twin law T a reflection whose twin mate is itself (up to the true group and Friedel) is untouched at every twin fraction. For each index-2 subgroup H of the adopted point group, those are the reflections centric in the group and acentric in H: centric if the operators the group adds over H are real, acentric if they are a twin law or a pseudo-symmetry - the one intensity statistic that still separates the two at fraction 0.5, where every operator statistic reads "real". Read on the P1 cross-check merge: epsilon-1 reflections in shells with <I/sigma> >= 5 (noise inflates every class towards centric), each class normalised against its own mean in bins of ~100 reflections and within the two phase classes of a detected pseudo-translation, Wilson outliers above E^2 = 20 dropped. Reported per subgroup: the added operators, n, <|E^2-1|> +- SE read absolutely against 0.968 / 0.736, and the centric-over- acentric Wilson log-likelihood in nats with both densities convolved with each reflection's error (flooring E^2 at its sigma instead read a genuine 1.2 A lysozyme zone as acentric), with the acentric control beside it. Log, report prose and TWIN_ZONE_n keys. Nothing reads it back; no decision changes. On the reference sets: 6toc P4222, all three subgroups centric (1.04-1.07, +253 to +534 nats); 6iu9 P3121 over P31 acentric (0.789, -294 nats); 5j23 R32 over R3 acentric (0.805, -304 nats, tNCS-class normalised); lysozyme P41212 centric (0.90, +476 to +1297); a P21 myoglobin centric (0.930, +135). Co-Authored-By: Claude Opus 5 (1M context) <noreply@anthropic.com>	2026-09-20 18:45:03 +02:00
leonarski_fandClaude Opus 5	99123f33df	Twinning: normalised L-test, and one verdict read in every Laue class ... The L-test now divides each intensity by its resolution-shell mean before forming pairs, over the shells whose <I/sigma> reaches 1 (the floor the second moment already used). Two index steps are not the same resolution, and on a small cell with a steep fall-off the raw pairs read <|L|> up to 0.08 high: an untwinned crystal 0.568 and a partial twin 0.427 where phenix.xtriage reads 0.486 and 0.360. Normalised, the four reference merges (6toc, 6iu9, 5j23, a lysozyme) agree with xtriage within 0.02 (0.487, 0.376, 0.374, 0.480). Selection stays by shell, never by the reflection's own I/sigma, which biases <|L|> down. Equal-count shells were tried for the second moment and widen its gap to xtriage, so the shells are kept. The L-test is no longer switched off in holohedral Laue classes. Merging I(h) with I(Th) under a false operator gives (I(h)+I(Th))/2 for every twin fraction, the perfect-twin distribution, so <|L|> < 0.42 there is reported as an adopted operator averaging unequal intensities (promotion suspect, or a twin law absorbed into the point group) - a warning, not a veto. Over 42 holohedral merges of the corpus the genuine ones read 0.436-0.513, the over-promoted H3 twin 0.374, and one ~490 A-axis crystal 0.365. The verdict is one line (TwinningVerdictLine) used by the stats text, the report prose, the summary row, the warning and the viewer; a new TWINNING_VERDICT key names it. The twin fraction comes from the statistic that carries the verdict (the L-test unless the call rests on the second moment alone), is not quoted from a second moment under a detected pseudo-translation, and is not quoted at all on a merge under a suspect operator. The pre-search numbers (measured on the P1 search merge) are user-visible, are measured with that merge's own pseudo-translation declared, and leave out the reflections the lattice centring extinguishes - an R lattice in its hexagonal cell otherwise pairs present with absent reflections (5j23: 0.633 with them, 0.40 without). Report-only: no space-group decision, merge or intensity changes. Co-Authored-By: Claude Opus 5 (1M context) <noreply@anthropic.com>	2026-09-20 18:45:03 +02:00
leonarski_f	9aae0c2ba7	v1.0.0-rc.169 (#79) ... * Building Jungfraujoch no longer needs zlib or Eigen installed on the machine, and the dependencies the build fetches are pinned and updated to current releases. * rugnux: improvements in indexing, lattice selection and geometry post-refinement, which index crystals that previously returned no lattice and keep the better of the two geometries a run measures. * rugnux: improvements in beam-centre measurement, beam-stop detection and space-group determination. * rugnux: the unit cell reported with a determined space group now obeys that group - a cell whose symmetry was confirmed from the intensities is re-refined under it, and a cell the group cannot describe is reported with a warning rather than as it stands. * rugnux drops the stretches of a rotation sweep whose removal measurably improves the merged intensities and reports what became of every frame, and decides the resolution cut on the crystal's own diffraction rather than on its ice rings. * The rugnux results report is machine-readable - every line that is not `KEY= value` data starts with `#` - and states the build it was written by, its authorship and its terms of use (`REPORT_VERSION= 8`). * `jfjoch_viewer`: improvements in the file manager (CBF frames beside HDF5 datasets, a remembered root), the dataset plots, the inspector and the image statistics, plus a settable font size, a view of the rugnux results report, usable performance over a remote display (`ssh -X`) and a reset of all settings to defaults; the reciprocal-space window is removed. * Broker fixes around DECTRIS collections and dark-mask calibration: re-initialising after a run that never started no longer freezes the broker, a cancelled calibration is abandoned instead of reported as done, and a collection whose start message never arrives ends by itself. Reviewed-on: #79 Co-authored-by: Filip Leonarski <filip.leonarski@psi.ch>	2026-09-15 17:09:31 +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_f	680c36c20d	v1.0.0-rc.166 (#76) ... * `rugnux --mode calibration` writes `<prefix>.json` beside the `.poni`, whose `dataset_settings` member is a `jfjoch_broker` `dataset_settings` body as it stands. * `rugnux` and `jfjoch_viewer` read PILATUS miniCBF sweeps natively, without conversion. * Masters written by other facilities open, including Eiger 1.x and third-party NXmx variants. * `rugnux` measures the beam centre on every run, and indexes with it when the file's value indexes nothing. * A detector swung out on a 2theta arm is placed where the file says it stands, and the calibration can hold the tilt fixed. * `rugnux` writes the unmerged MTZ by default, and a P1 merge beside it, so a wrong space group can be re-merged without reprocessing. * Significant improvements to symmetry handling in `rugnux`: the lattice, the point group, the setting and the systematic absences. * The `rugnux` report gives the resolution the CC1/2 fit reached, beside the range the reflections were written to. * The `rugnux` report gives the twinning statistics measured before the space group was decided, beside the ones measured after. * The `rugnux` report gives the strong-direction diffraction limit, and warns when CC1/2 is not monotone with resolution. * `rugnux` ranks screw axes on the evidence their absences carry, rather than on how many control reflections a candidate happens to have. * Twinning is no longer reported when the L-test contradicts it. * The `rugnux` report gives the detector tilt, the measured tilt and the direct beam beside the beam centre, and a post-refined beam centre is judged against the run's own measurement rather than the file's. * `--no-refine-tilt` holds the detector tilt at the value in the file, instead of zeroing it, when the calibration starts from the spots. * The `jfjoch_viewer` grid scan view draws the cells in the proportion of the scan steps, so the map has the shape of the scanned area. Reviewed-on: #76 Co-authored-by: Filip Leonarski <filip.leonarski@psi.ch>	2026-09-02 21:17:31 +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	451310f43d	v1.0.0-rc.158 (#68) ... 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. * Analysis: The azimuthal-integration solid-angle correction now follows the incidence angle to the detector normal (`cos^3` of that angle) instead of `cos^3(2*theta)`, so it is correct for a tilted detector and matches PyFAI `solidAngleArray` and MAX IV azint (unchanged for an untilted detector). Crystal geometry refinement (`XtalOptimizer`) no longer silently ignores an imported PONI `rot3` (rotation about the beam): it is applied as a fixed rotation in the residual so refinement stays consistent with the rest of the pipeline. Polarization and azimuthal binning already honoured `rot3` through the full PONI rotation. * jfjoch_viewer: Open datasets on the WSL2/UNC filesystem (paths starting `\\`); write processing outputs next to the input file, with a Browse button and independent `_process.h5` / merged `.mtz`/`.cif` toggles; and show the determined space group in the merge-statistics window. * rugnux: Accept an absolute `-o` output prefix in offline processing. * Packaging: The self-contained Linux viewer `.tgz` now bundles cuFFT, so it runs without a system CUDA toolkit (`.deb`/`.rpm` are unchanged, distro-managed). * Docs: Bring the analysis references up to date with the code. `docs/CPU_DATA_ANALYSIS.md` now reflects the unified profile-fit Bragg integration engine, multi-lattice indexing, azimuthal phi binning, the radial parallax/bandwidth profile with sub-pixel centring, the rot3d capture-fraction handling and the automatic CC1/2 resolution cutoff, and drops the descriptions of features that were never implemented (French-Wilson amplitudes, the still excitation-error partiality model); `docs/RUGNUX.md` documents the new `--resolution-cutoff`/`--resolution-cc-target`/`--resolution-shells`, `--min-captured-fraction`, `--mosaicity`, `--reference-column`, the azimuthal correction toggles and the geometry-override options, and corrects the `-N` default. The outdated in-source design notes (ICE_RING_DETECTION, BRAGG_INTEGRATION_ENGINE, NEXTGEN_INTEGRATOR) are removed.Reviewed-on: #68 Co-authored-by: Filip Leonarski <filip.leonarski@psi.ch>	2026-07-12 19:42:29 +02:00
leonarski_f	54c0100e8e	v1.0.0-rc.157 (#67) ... 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: Rebrand the offline data-processing subsystem as `rugnux` and consolidate all offline analysis into the single `rugnux` binary - `jfjoch_process` is now `rugnux`, the former `jfjoch_azint` is now `rugnux --azint-only`, and `jfjoch_scale` is now `rugnux --scale` (see the new docs/NAMING.md and docs/RUGNUX.md). Scaling and merging are on by default for rotation and stills (`--no-merge` disables them), replacing the previous opt-in `-M, --scale-merge`. * rugnux: CLI fixes - default `-N` to all hardware threads, parse numeric option arguments strictly (reject non-numeric or trailing input instead of silently yielding 0), require `--wavelength > 0`, and correct the reproduced command line and `--scale` reference-cell handling. * rugnux: De-novo space-group improvements - recover genuine high symmetry and centred Bravais lattices from intensities, add an automatic CC1/2 high-resolution cutoff, and report L-test twinning statistics. * rugnux: Index weakly-diffracting low-resolution rotation data that previously failed (e.g. F-cubic crystals that diffract only to ~4 A on a detector reaching ~1.5 A). The per-frame indexing gate now measures the indexed fraction only within the resolution range the lattice actually diffracts to, so the many sub-diffraction ice/noise spots no longer make the fraction floor unreachable; the two-pass first pass tries several image-sampling schemes (spread across the whole rotation vs a consecutive wedge whose native stride keeps a reflection's rocking curve continuous, letting the FFT resolve a long axis) and keeps the one that indexes the most frames; and the de-novo space-group search no longer discards all reflections (and crashes) when every resolution shell falls below <I/sigma> = 1. * rugnux: Lower the low-resolution R-meas for strongly-diffracting rotation data - drop edge-of-sweep truncated fulls whose rocking curve was captured below `--min-captured-fraction` (default 0.7 for rotation), and report R-meas only over the observations kept by outlier rejection (matching XDS). The 0.7 default also strips the partiality-extrapolated fulls that dominate the intensity second moment on weakly-diffracting crystals, so the de-novo space-group search is no longer starved by the error-model I/sigma floor and recovers the correct symmetry (e.g. the F-cubic Benas crystals: Benas_3 -> F432, Benas_7 -> P6122, instead of P4/P1); on the reference battery every other crystal keeps its space group. * rugnux: Write the refined geometry (beam, tilt, axis) to _process.h5 and place non-standard mmCIF items under a reserved `jfjoch` prefix. * jfjoch_broker: Ordinary acquisition failures (receiver/writer/analysis problems, missed packets, writer disconnect) now return to the Idle state with an Error-severity message, so a run can be retried without an expensive re-initialisation; only failures that leave the detector in an undefined state (new JFJochCriticalException, e.g. PCIe/FPGA faults) go to the Error state and force re-initialisation. * jfjoch_broker: A synchronous /start now reports its failure to the HTTP caller instead of returning HTTP 200, and an incomplete or truncated dataset (missing packets, writer disconnect) is reported as an error rather than a "reduce frame rate" warning. * jfjoch_broker: Drop uncollected placeholder rows (number = -1) from the scan_result REST endpoint. * jfjoch_broker: Fix the inverted per-image compression ratio reported by the Lite receiver (was compressed/uncompressed instead of uncompressed/compressed). * jfjoch_broker: Bragg integration adds a quantization-noise variance floor with a box-sum fallback, and treats the type-maximum marker as an invalid pixel for unsigned image types. * jfjoch_writer: Detect file-overwrite conflicts at start for back-channel transports, and reset the writer when end-of-collection finalisation fails. * jfjoch_viewer: Preview overlays follow the geometry (resolution/ROI arcs, true beam centre, predictions, coral secondary-lattice spots, legend), add save-as-JPEG, and fix an HTTP live-follow memory leak. * Frontend: Improved aesthetics and usability, and added in-browser pixel-mask and JUNGFRAU-pedestal visualisation. * CI: Name the Windows installer jfjoch-viewer-* instead of jfjoch-*.Reviewed-on: #67 Co-authored-by: Filip Leonarski <filip.leonarski@psi.ch>	2026-07-11 07:19:11 +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