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The observation model said its L term was the prescaling correction, and that predictions carry its reciprocal as prescaling_corr. That was true when that one field held everything. It has since been narrowed to Lorentz x polarization, with the sensor's efficiency and the flight path carried beside it, and every site that corrects an intensity multiplies all three - the scaling fits, the merge ingest, the anisotropy analysis and the unmerged export alike. So the model term is the product, not the first factor of it, and a reader implementing against that page would have applied a third of the correction. The header comment on the efficiency factor had the same fossil: it said the total correction is prescaling_corr * qe_corr, written before the flight path existed. The comment two fields below it already said all three, so the file disagreed with itself. Co-Authored-By: Claude Opus 5 <noreply@anthropic.com> Claude-Session: https://claude.ai/code/session_01EFEJG6WBQv8th4UJFNe53N
84 lines
3.9 KiB
C++
84 lines
3.9 KiB
C++
// SPDX-FileCopyrightText: 2025 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 <cstdint>
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#include <optional>
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#include <cmath>
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#include "SpotToSave.h"
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struct Reflection {
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int32_t h;
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int32_t k;
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int32_t l;
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float image_number; // Can be in-between for 3D integration
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float delta_phi_deg; // phi angle from XDS - difference from middle of current frame (NOT an absolute angle)
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float predicted_x;
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float predicted_y;
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float observed_x;
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float observed_y;
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float d;
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float I;
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float bkg;
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float var_bkg; // non-signal (background) part of sigma^2, carried to the merge
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float sigma;
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float dist_ewald;
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// The reciprocal Lorentz factor (rotation only - a still's Lorentz factor is one) times the
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// reciprocal polarization factor, and nothing else. This is what LP means everywhere in the
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// field, and it is what the CBOR key "rlp" and the HDF5 dataset "lp" store the reciprocal of.
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// What it is not is a scale: the fitted per-image scale and the partiality stay out of it and
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// are divided in separately below. (Named after DIALS's prescaling_correction.)
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float prescaling_corr;
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// The sensor's angle-dependent efficiency, QE(0)/QE(alpha): always <= 1, and exactly 1 where the
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// sensor is opaque or its material and thickness are unknown. It is carried BESIDE
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// prescaling_corr rather than inside it, because LP and detector response are two different
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// things and every file the field reads keeps them apart. It is one of the three factors whose
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// product is the total deterministic correction - see flight_corr below, which arrived after
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// this comment was written and made "the two" wrong. Defaulted to 1 so a reflection read from a
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// file written before this existed is a no-op rather than a zero.
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float qe_corr = 1.0f;
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// The air in the sample-to-pixel flight path, exp(D/L * (1/cos(alpha) - 1)): always >= 1, and
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// exactly 1 when the air correction is switched off. Carried beside the two above for the same
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// reason they are carried apart - it is neither beam geometry nor detector response but the
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// medium in between, and unlike either of them it is set by the flight distance. The total
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// deterministic correction on a reflection is prescaling_corr * qe_corr * flight_corr, and every
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// site that corrects an intensity multiplies all three. Defaulted to 1 so a reflection read
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// from a file written before this existed is a no-op rather than a zero.
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float flight_corr = 1.0f;
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float partiality; // fraction of the reflection recorded in the sampled (rocking) slice
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float zeta;
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float image_scale_corr; // I_true = image_scale_corr * I; = prescaling_corr * qe_corr * flight_corr / (partiality * image_scale)
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bool observed = false;
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bool on_ice_ring = false; // sits on a hexagonal-ice powder ring: excluded from scaling, kept for merging
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};
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struct MergedReflection {
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int32_t h = 0;
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int32_t k = 0;
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int32_t l = 0;
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float I = NAN;
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float sigma = NAN;
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float I_half[2] = {NAN, NAN};
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float sigma_half[2] = {NAN, NAN};
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float d = 0.0;
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bool rfree_flag = false;
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float F = NAN; // French-Wilson amplitude |F| (filled by ApplyFrenchWilson at end of merge)
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float sigmaF = NAN; // its sigma
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// Anomalous (Bijvoet) split of this reflection's own observations, kept even when the merge is
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// Friedel-averaged (I above is the Friedel mean). Lets I(+)/I(-) be written and CCano reported by
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// default without scaling anomalously; NaN when a hand was not measured or for centrics.
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float I_plus = NAN;
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float sigma_plus = NAN;
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float I_minus = NAN;
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float sigma_minus = NAN;
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// French-Wilson amplitudes of the two hands (filled by ApplyFrenchWilson from I_plus/I_minus).
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float F_plus = NAN;
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float sigmaF_plus = NAN;
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float F_minus = NAN;
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float sigmaF_minus = NAN;
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};
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