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Jungfraujoch/image_analysis/rotation_indexer/RotationIndexer.h
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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

70 lines
2.9 KiB
C++

// SPDX-FileCopyrightText: 2025 Filip Leonarski, Paul Scherrer Institute <filip.leonarski@psi.ch>
// SPDX-License-Identifier: GPL-3.0-only
#pragma once
#include <memory>
#include <vector>
#include <mutex>
#include "../../common/DiffractionSpot.h"
#include "../../common/DiffractionExperiment.h"
#include "../indexing/IndexerThreadPool.h"
#include "../lattice_search/LatticeSearch.h"
struct RotationIndexerResult {
CrystalLattice lattice;
std::vector<CrystalLattice> extra_lattices;
LatticeSearchResult search_result;
DiffractionGeometry geom;
std::optional<GoniometerAxis> axis;
// The same lattice refined WITHOUT the metric symmetry (triclinic P), when there is one to
// compare against. The Bravais class is decided on the UNREFINED FFT candidate against a fixed
// angular tolerance, so a pseudo-symmetric cell can be promoted a class too far and the
// constraint then snaps a real angle to the ideal one; here the caller can settle that on a
// statistic the accumulated-spot fraction is too blunt for. Null on the alternative itself.
std::shared_ptr<RotationIndexerResult> unconstrained;
};
class RotationIndexer {
mutable std::mutex m;
const DiffractionExperiment& experiment;
constexpr static size_t max_spots = 10000;
constexpr static size_t max_spots_per_image = 200;
const bool index_ice_rings;
std::vector<std::vector<SpotToSave>> v_;
// Per-image rotation angle (mid-exposure, deg) supplied by the caller; falls back to the
// goniometer evaluated at the image index when not given.
std::vector<std::optional<float>> angle_deg_;
std::optional<GoniometerAxis> axis_;
const DiffractionGeometry geom_;
DiffractionGeometry updated_geom_;
LatticeSearchResult search_result_;
std::vector<CrystalLattice> extra_lattices_;
std::shared_ptr<RotationIndexerResult> unconstrained_;
IndexerThreadPool &indexer_;
size_t accumulated_spots = 0;
std::optional<CrystalLattice> indexed_lattice;
public:
RotationIndexer(const DiffractionExperiment& x, IndexerThreadPool& indexer);
// angle_deg is the image's mid-exposure rotation angle; if omitted, the goniometer angle at
// `image` is used (only valid when `image` is the goniometer's own image index).
void ProcessImage(int64_t image, const std::vector<SpotToSave>& spots,
std::optional<float> angle_deg = std::nullopt);
void RunIndexing();
std::optional<RotationIndexerResult> GetLattice() const;
void ForceLattice(const CrystalLattice& lattice);
// Adopt a complete result (lattice + refined geometry/axis/symmetry) found by another indexer -
// used when several first-pass sampling schemes are run and the best is selected.
void ForceResult(const RotationIndexerResult& result);
// True once the accumulation buffer is full (used to stop feeding a consecutive-frame scheme).
[[nodiscard]] bool AccumulationFull() const;
};