Jungfraujoch/image_analysis/bragg_integration/BackgroundAperture.h

// SPDX-FileCopyrightText: 2026 Filip Leonarski, Paul Scherrer Institute <filip.leonarski@psi.ch>
// SPDX-License-Identifier: GPL-3.0-only

#pragma once

#include <cstddef>
#include <cstdint>
#include <vector>

#include "../../common/DetectorModules.h"
#include "../../common/DiffractionGeometry.h"
#include "../../common/DiffractionSpot.h"
#include "../image_preprocessing/ImagePreprocessorBuffer.h"
#include "RingBackground.h"

// How far out the background ring should reach, measured on apertures with nothing in them.
//
// The ring mean stands in for the background under the signal disk. A wider ring averages more pixels,
// so its own noise falls; but it also reaches further from the reflection, so whatever the background
// does between the disk and the ring - a curved solvent ring, the tile structure of a fibre-optic CCD,
// the tails of reflections nobody predicted - enters the intensity as a bias. Which of the two wins is
// a property of the detector and the sample, not a constant: on a pixel detector counting a fraction of
// a photon per pixel the noise wins and the widest ring is best, on a binned CCD reading hundreds of
// ADU a pixel the structure wins and the narrowest is.
//
// So it is measured. Apertures are laid on a grid over pre-scan frames, away from every spot found; on
// each, the mean of the r1 disk and the mean of the r2..r3 ring are taken for every candidate r3, and
// the run keeps the r3 whose ring predicts the disk best - the smallest mean square of the difference.
// With nothing in the aperture the difference is exactly the error the ring makes in the background of
// a reflection: its noise plus its bias. The disk's own noise is the same for every candidate, so it
// does not move the choice. The ring is clipped as the integrator clips it (high side, at
// mean + nsigma * sqrt(gain * mean)).
//
// The same apertures also say whether the radial background-curvature correction helps: each difference
// is taken a second time with the correction applied as the integrator applies it - the ring's clip
// following the frame's own ring background (RingBackground), and that background averaged over the
// ring pixels the clip kept minus over the disk's, which is what the integrator takes off a reflection
// (BraggCurveCorrection).
// Where the background really is a function of the radius the corrected ring predicts the disk better;
// where it is not - a strongly polarised beam, panels of different response - it predicts it worse, and
// the run measures which. On stills the ring is chosen on the plain differences first, so its reach does
// not rest on the radial model; the correction is then kept where it improves that ring. Rotation measures
// every stencil the spot width can give it, and reads the one it gets.
namespace background_aperture {

// The squared disk-minus-ring differences, summed per candidate r3 over every aperture measured: plain,
// and with the radial correction (counted separately: a frame without a ring background adds none).
struct Tally {
    std::vector<double> sum_d2, sum_d2_radial;
    // Sum of the squared per-aperture change the correction makes to d^2, for the standard error of
    // the paired comparison (RadialZ).
    std::vector<double> sum_dd2;
    size_t apertures = 0, apertures_radial = 0;
    void Add(const Tally &other);
    // The mean square difference of each candidate, plain or corrected; empty where nothing was measured.
    [[nodiscard]] std::vector<double> MeanSquare(bool radial) const;
    // How many standard errors the correction lowers candidate k's mean square by, over the apertures
    // measured both ways (positive: the correction helps).
    [[nodiscard]] double RadialZ(size_t k) const;
};

// A signal disk r1, the inner edge of its ring r2, and the candidate outer edges r3.
struct Stencil {
    float r1 = 0.0f, r2 = 0.0f;
    std::vector<float> r3;
};

// The candidate outer radii: from r2 + 2 up to max_r3, one pixel apart.
[[nodiscard]] std::vector<float> CandidateR3(float r2, float max_r3);

// The apertures of one frame, appended to `tally`. Centres lie on a grid over the frame, and an aperture
// is used only where every pixel out to the largest candidate is readable and no found spot is within
// that radius plus SPOT_CLEARANCE_PX of its centre. `rings` is this frame's ring background, or empty;
// `geometry` and `modules` place the pixels on the plane to read it at their resolution.
void MeasureFrame(ImagePreprocessorBuffer &image, int width, int height,
                  const std::vector<DiffractionSpot> &spots, float r1, float r2,
                  const std::vector<float> &r3, float clip_nsigma, float gain,
                  const RingBackground &rings, const DiffractionGeometry &geometry,
                  const DetectorModules &modules, Tally &tally);

// Whether the radial correction makes candidate k's ring predict the disk better - its mean square
// difference lower by at least the fraction min_gain - on apertures that were all measured both ways.
[[nodiscard]] bool RadialHelps(const Tally &tally, size_t k, double min_gain = 0.0);

// The part of the background error the correction must take away on a rotation run. A still has no other
// correction, so any gain is taken there; a rotation run already corrects the frames whose ice score shows
// a smooth ring, and the frame's curve on every frame replaces that only for a clear gain. Measured: on
// photon-counting sweeps the apertures gain 0.1-5% (z 3-4) and every image corrected costs ISa and
// anomalous signal; where it pays - home-source CCD rings, a smooth ice ring - they gain 13-31%.
constexpr double ROTATION_RADIAL_MIN_GAIN = 0.10;

// The candidate with the smallest mean square difference, or -1 where nothing was measured.
[[nodiscard]] int Best(const std::vector<double> &mean_square);

constexpr float SPOT_CLEARANCE_PX = 4.0f;
// At most this many apertures a frame: a 16 Mpx detector would otherwise lay twenty thousand.
constexpr size_t MAX_APERTURES_PER_FRAME = 2000;

}   // namespace background_aperture