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d28db19ab1 |
Space-group search: judge a screw axis against its own axial row
A reflection the group predicts absent counted as a violation when
I/sigma > 3 AND E^2 = I/<I>(shell) > 0.3. Neither half survives contact
with real data:
* merged sigma is floored at b|I|, so merged I/sigma saturates at ISa
for nearly every reflection - the I/sigma half is an on/off switch
keyed on ISa vs 3, not a per-reflection test. On one crystal the
absent class read <I/s> 4.10 against 3.73 for the present class while
being genuinely extinct;
* <I>(shell) decays with resolution while a systematically-absent
reflection keeps a small NON-decaying residual (background / profile
leakage), so absent reflections drift over an absolute E^2 cut at high
resolution. That cost a tetragonal 42_12 crystal its 4_1: 18 of its 47
absent 00l crossed the cut, all beyond 3.7 A, at absolute intensities
identical to the low-resolution ones correctly judged absent, while
their l=4n row-mates sat 20-60x higher at the same resolution.
A screw extinguishes only the reflections that lie ON its axis, so the
fair yardstick is the rest of that same row. The threshold is now
0.3 * max(1, median E^2 of the reflection's own row), the row being the
gcd-reduced reciprocal-space direction and the control class the same-row
reflections the group predicts present. Floored at 1, so it only ever
relaxes: a screw can be recovered by it, never lost.
Per row, not pooled. A 4_1 along c and a 2_1 along a are separate
conditions with separate controls; pooling let the weak a/b rows (median
E^2 ~0.5) set the threshold for a strong c row (8.4) and the rescue never
fired.
The candidate table now reports the screw evidence (median E^2 of the
absent class and of its rows) - the <I/s> columns are the centering
evidence and say nothing about screws, for the sigma-floor reason above.
Rotation battery, 33 crystals: 31 decisions bit-identical, the 42_12
crystal recovers its 4_1 (0 violations, row E^2 8.4 vs absent 0.12), and
one crystal with a long axis and heavy 00l overlap moves to a 4_1 group at
exactly 10.0% violations - marginal, and its sister crystal of the same
form sits at 13.3% and does not move. Real screws now span 0-9.3%
violations, so max_absent_violation_fraction cannot be tightened below
0.10 without risking a genuine one.
Co-Authored-By: Claude Opus 5 (1M context) <noreply@anthropic.com>
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67dca388bd |
v1.0.0-rc.160 (#70)
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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> |
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d6389e12da |
v1.0.0-rc.156 (#66)
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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> |
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166fcdb68f |
v1.0.0-rc.131 (#39)
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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.124. * jfjoch_broker: Fix bug in saving JUNGFRAU calibration (pedestal/pedestalRMS) * jfjoch_viewer: Fix calibration (pedestal) images being open flipped * jfjoch_process: Add space group detection (EXPERIMENTAL) Reviewed-on: #39 |