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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: 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>
177 lines
10 KiB
C++
177 lines
10 KiB
C++
// SPDX-FileCopyrightText: 2026 Filip Leonarski, Paul Scherrer Institute <filip.leonarski@psi.ch>
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// SPDX-License-Identifier: GPL-3.0-only
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#pragma once
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#include <optional>
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#include "JFJochException.h"
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// How the high-resolution cutoff for the written reflections and the reported shell table is chosen
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// when no explicit --scaling-high-resolution is given. Off = keep the full (detector-edge) range;
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// CCHalfLogistic = fit the CC1/2 fall-off and cut one shell past cc_target (DIALS-style, generous).
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enum class ResolutionCutoffMethod { Off, CCHalfLogistic };
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class ScalingSettings {
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bool refine_wedge = false;
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bool merge_friedel = true;
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std::optional<double> high_resolution_limit_A;
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// Low-resolution limit for scaling and merging. Reflections coarser than this are behind or
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// beside the beam stop and are measured on a background the stop has eaten into; past 50 A a
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// large share of them come out negative. 50 A is what XDS's own configurations use, so keeping
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// it here is also what makes the two comparable at the coarse end.
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std::optional<double> low_resolution_limit_A = 50.0;
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std::optional<double> wedge_for_scaling;
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std::optional<double> forced_mosaicity; // diagnostic: fix the scaling mosaicity (deg) instead of the per-image seed
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double min_partiality = 0.02;
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// Capture-aware systematic uncertainty for the rot3d combine: a full reconstructed from only
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// a fraction f<1 of its rocking curve is extrapolated, and the unobserved (1-f) carries a
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// systematic error ~coeff*(1-f)*I that plain counting sigma misses. 0 = off (baseline).
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double capture_uncertainty_coeff = 0.0;
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// Full-level captured-fraction floor for the rot3d combine: drop a reconstructed full whose rocking
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// curve was only fractionally captured (sum of its partials' partiality < this). Distinct from
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// min_partiality, which gates individual partials; this gates the assembled full. 0 = off (baseline).
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double min_captured_fraction = 0.0;
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double min_cc_for_image = 0.0;
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// Exclude observations whose Lorentz geometry |zeta| falls below this from the DE-NOVO space-group
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// search merge only (see RotationScaleMerge::search_min_zeta). 0 = off.
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double search_min_zeta = 0.0;
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double outlier_reject_nsigma = 0.0; // per-observation merge outlier rejection (XDS/DIALS-style); 0 = off, e.g. 6 enables
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// Scale fulls: after the rotation 3D combine, refit a per-frame scale on the combined fulls (XDS
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// order). Only used by the rotation path (RotationScaleMerge).
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bool scale_fulls = false;
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// Correction surfaces fitted on the rot3d fulls after scale-fulls: a decay (per-run Debye-Waller B)
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// and an absorption surface (over the diffracted-beam direction in the goniometer frame). Both are
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// cross-validated, so they no-op when their systematic is absent - hence ON by default (they only ever
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// help or do nothing). No-op without rot3d. Set false to disable both.
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bool correction_surfaces = true;
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// Absorption-surface refinement iteration count (used when correction_surfaces is on).
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int absorption_iter = 3;
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// Physical partiality post-refinement for the STILLS merge (StillsPartialityRefine): refine a per-crystal
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// orientation tilt against the running merge, recompute each reflection's partiality from the refined
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// geometry (angular Ewald-proximity model), and re-scale/merge - the "full model" for stills. ON by
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// default (helps mono stills, neutral on pink beam, tames weak data via a soft prior). rugnux
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// --simple-stills turns it OFF, reverting to treating every reflection as a full (p = 1, single pass).
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bool stills_partiality_refine = true;
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// Expected-variance merge weighting for the STILLS merge (MergeOnTheFly). When combining a reflection's
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// redundant observations by inverse variance, rebuild the Poisson signal part of each observation's
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// variance at the reflection's EXPECTED <I> instead of the observation's own intensity. Weighting by an
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// observation's own sigma^2 biases the inverse-variance mean low at <1 photon (an up-fluctuated
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// observation gets a larger sigma and is over-downweighted). Default on - it mirrors the rotation combine
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// (RotationScaleMerge::process_rawrun), which already does this, and is R-free-neutral on strong data and
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// better on weak. --no-expected-variance-merge restores the old observed-sigma weighting.
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bool expected_variance_merge = true;
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// Minimum measured ice strength (iceRingScore, 1 = no ice) before any ice-ring handling is applied
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// at all. The eleven fixed hexagonal bands cover 16-26% of the unique reflections at typical
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// resolutions REGARDLESS of whether the crystal has ice, so flagging unconditionally taxes clean
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// data for nothing. 0 disables the gate (always handle ice, the previous behaviour).
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// 1.5 is measured, not guessed: over 37 rotation crystals the score lands at 1.00-1.22 on the
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// thirty with no ice, 1.28-1.44 on four borderline ones whose ice-ring positions show no
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// azimuthally smooth elevation, and 2.08-2.37 on the three with confirmed ice - and a decoy null
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// (the identical statistic at ring positions where hexagonal ice cannot be) never exceeded 1.29.
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float ice_min_score = 1.5f;
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// The same gate on the SECOND ice channel: spots found on the hexagonal rings over the same q width
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// of ice-free flanks beside them (1 = spots spread evenly). This is what catches ice in large
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// crystallites, which diffracts as discrete spots and leaves the radial profile - and so
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// ice_min_score - flat. Also measured, not guessed: over 36 rotation crystals thirty read
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// 0.65-1.37 and a clean control 1.04, then 1.63/1.78 and a gap to 2.18-14.6 on the five whose
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// spots really do pile up on the rings. 0 disables this channel.
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float ice_min_spot_ratio = 2.0f;
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// Smooth the per-frame scale G across frames (centered moving average of log G) before the rot3d
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// combine, so a rocking event's partials share a consistent scale. Given as a ROTATION RANGE in
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// degrees (like XDS DELPHI), converted to an odd frame window from the oscillation step; this keeps
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// the smoothing physical (independent of frame slicing). 0 = off. A no-op without rot3d.
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double smooth_g_deg = 0.0;
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// Per-batch relative-B on the rot3d fulls (beyond the single global decay slope): bin frames into
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// rotation-range batches of this width in degrees and refine one relative Debye-Waller B per batch, so
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// NON-monotonic changes in scattering power across the run (absorption path, crystal slippage, dose
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// bursts) are corrected the resolution-flat per-frame G and the single decay slope both miss. Cross-
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// validated + zero-mean-anchored, so a no-op when absent. 0 = off. A no-op without rot3d.
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double relative_b_deg = 0.0;
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double rfree_fraction = 0.05;
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// Automatic high-resolution cutoff for the written reflections + reported shells (not the scaling
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// or the error model, and not the per-image _process.h5). Applied only when no explicit
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// high_resolution_limit_A is set - that manual limit always wins and disables the auto-cut.
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ResolutionCutoffMethod resolution_cutoff = ResolutionCutoffMethod::CCHalfLogistic;
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double resolution_cc_target = 0.30; // CC1/2 value defining the fall-off limit before the +1 shell
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int report_shell_count = 10; // number of resolution shells in the reported statistics table
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public:
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ScalingSettings& RefineRotationWedge(bool input);
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ScalingSettings& RotationWedgeForScaling(std::optional<double> input);
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ScalingSettings& MergeFriedel(bool input);
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ScalingSettings& HighResolutionLimit_A(double limit);
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ScalingSettings& HighResolutionLimit_A(std::optional<double> limit); // nullopt clears the limit
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ScalingSettings& LowResolutionLimit_A(std::optional<double> limit); // nullopt clears the limit
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ScalingSettings& MinPartiality(double min_partiality);
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ScalingSettings& ForcedMosaicity(std::optional<double> input);
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ScalingSettings& CaptureUncertaintyCoeff(double input);
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ScalingSettings& MinCapturedFraction(double input);
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ScalingSettings& MinCCForImage(double min_cc_for_image);
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ScalingSettings& SearchMinZeta(double search_min_zeta);
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ScalingSettings& OutlierRejectNsigma(double input);
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ScalingSettings& ScaleFulls(bool input);
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ScalingSettings& AbsorptionIter(int input);
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ScalingSettings& CorrectionSurfaces(bool input);
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ScalingSettings& StillsPartialityRefine(bool input);
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ScalingSettings& ExpectedVarianceMerge(bool input);
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ScalingSettings& IceMinScore(float input);
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ScalingSettings& IceMinSpotRatio(float input);
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ScalingSettings& SmoothGDegrees(double input);
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ScalingSettings& RelativeBDegrees(double input);
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ScalingSettings& RfreeFraction(double input);
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ScalingSettings& ResolutionCutoff(ResolutionCutoffMethod input);
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ScalingSettings& ResolutionCCTarget(double input);
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ScalingSettings& ReportShellCount(int input);
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[[nodiscard]] bool GetRefineWedge() const;
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[[nodiscard]] double GetMinMosaicity() const;
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[[nodiscard]] double GetDefaultMosaicity() const;
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[[nodiscard]] double GetMaxMosaicity() const;
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[[nodiscard]] double GetMinWedge() const;
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[[nodiscard]] std::optional<double> GetRotationWedgeForScaling() const;
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[[nodiscard]] double GetMaxWedge() const;
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[[nodiscard]] bool GetMergeFriedel() const;
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[[nodiscard]] std::optional<double> GetHighResolutionLimit_A() const;
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[[nodiscard]] std::optional<double> GetLowResolutionLimit_A() const;
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[[nodiscard]] double GetMinPartiality() const;
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[[nodiscard]] std::optional<double> GetForcedMosaicity() const;
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[[nodiscard]] double GetCaptureUncertaintyCoeff() const;
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[[nodiscard]] double GetMinCapturedFraction() const;
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[[nodiscard]] double GetMinCCForImage() const;
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[[nodiscard]] double GetSearchMinZeta() const;
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[[nodiscard]] double GetOutlierRejectNsigma() const;
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[[nodiscard]] bool GetScaleFulls() const;
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[[nodiscard]] int GetAbsorptionIter() const;
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[[nodiscard]] bool GetCorrectionSurfaces() const;
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[[nodiscard]] bool GetStillsPartialityRefine() const;
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[[nodiscard]] bool GetExpectedVarianceMerge() const;
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[[nodiscard]] float GetIceMinScore() const;
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[[nodiscard]] float GetIceMinSpotRatio() const;
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[[nodiscard]] double GetSmoothGDegrees() const;
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[[nodiscard]] double GetRelativeBDegrees() const;
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[[nodiscard]] double GetRfreeFraction() const;
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[[nodiscard]] ResolutionCutoffMethod GetResolutionCutoff() const;
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[[nodiscard]] double GetResolutionCCTarget() const;
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[[nodiscard]] int GetReportShellCount() const;
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};
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