Jungfraujoch/image_analysis/spot_finding/SpotUtils.h

// SPDX-FileCopyrightText: 2025 Filip Leonarski, Paul Scherrer Institute <filip.leonarski@psi.ch>
// SPDX-License-Identifier: GPL-3.0-only

#pragma once

#include "../../common/DiffractionSpot.h"

void GenerateSpotPlot(DataMessage &msg, const std::vector<SpotToSave> &spots, float d_min_A);

void CountSpots(DataMessage &msg,
                const DiffractionExperiment& experiment,
                const std::vector<DiffractionSpot> &spots,
                float d_min_A);

void CountSpots(DataMessage &msg,
                const std::vector<SpotToSave> &spots,
                float d_min_A);

float CountIceRingControlSpots(const std::vector<SpotToSave> &spots, float half_width_q_recipA);

void MarkIceRings(std::vector<SpotToSave> &spots, float tolerance_q_recipA);

// Flag every spot sitting within tolerance of one of the given ring positions (q = 2*pi/d). The same
// flag MarkIceRings sets, because it means the same thing downstream: a spot that belongs to a powder
// ring and not to this crystal.
void MarkRings(std::vector<SpotToSave> &spots, const std::vector<float> &rings_q_recipA,
               float tolerance_q_recipA);

// What a POOLED spot list says about powder contamination: a crystalline phase other than the
// crystal, diffracting as rings the crystal's own reflections sit among. Hexagonal ice has a fixed
// list of rings and MarkIceRings above; nothing else that powders does - a shower of microcrystals
// around the crystal, salt out of the cryoprotectant, a phase nobody expected - and on such a pattern
// the contaminant's spots can outnumber the crystal's several times over in every frame.
//
// A ring is a q bin holding far more spots than the smooth spot-density fall-off around it. The
// baseline is a running median over a window wide compared with a ring, so it follows that fall-off
// without following the rings themselves. Pool over frames spread across the sweep: a powder ring is
// on every frame and the crystal's own rows are not, so pooling sharpens the rings and flattens
// everything else.
struct PowderRings {
    // Ring centres, q = 2*pi/d. Empty on a pattern that shows no rings, which is most of them.
    std::vector<float> rings_q_recipA;
    // The share of the pooled spots that the rings hold OVER the baseline - what the contaminant
    // contributes, not what happens to lie in a ring band. 0 where there is nothing.
    float spot_fraction = 0.0f;
    // How far the rings can be told apart, in A. A powder's rings crowd together as q grows, and past
    // the point where ring bins are the majority of bins the baseline is itself made of rings and a
    // ring no longer measures as one. Nothing finer than this can be separated from the crystal, so
    // it is the resolution an indexing pass can be asked to trust on such a pattern. Absent where the
    // rings stay separable over the whole range, which is the ordinary case.
    std::optional<float> resolved_to_d_A;
};
PowderRings MeasurePowderRings(const std::vector<float> &spot_q_recipA, float half_width_q_recipA);

// The resolution (A) that this fraction of a pooled spot list lies COARSER than. A first pass that
// stops here is given that share of the spots, whatever the detector reaches and whatever the
// crystal's fall-off looks like - so it scales to any dataset without a resolution written into the
// program. Returns nothing on a pool too small to have quantiles.
std::optional<float> SpotResolutionQuantile(const std::vector<float> &spot_q_recipA, float fraction);

// Keep the strongest `count` spots. With deprioritise_ice, spots on the hexagonal ice bands are ordered
// last and so are the first to go; pass false where the run has no measurable ice, in which case the
// flag marks ordinary reflections and ordering on it would discard good data.
void FilterSpotsByCount(std::vector<SpotToSave> &input, int64_t count, bool deprioritise_ice);

void FilterSpuriousHighResolutionSpots(std::vector<SpotToSave> &spots, float threshold);

// How far the SCALED AND MERGED data from a run of images like this one are expected to reach, in A,
// from the spots of this one image alone. Nothing else - no lattice, no integration, no merge.
//
// The spots' intensity-weighted resolution distribution falls off at the crystal's own rate, and a
// quantile taken near the middle of that fall-off measures that rate. The far end of the distribution
// does not: the highest-resolution spot found says where DETECTION stops, which moves with the
// exposure and with how many reflections the unit cell puts on the frame. Merging then reaches a fixed
// factor further in 1/d than the quantile, because averaging many observations goes on measuring
// intensities that one image cannot detect.
//
// The answer is deliberately NOT limited to what this detector records. The quantile sits in the
// middle of the fall-off, well inside the recorded range, so it goes on measuring the crystal when
// the detector stops before the diffraction does - which is the case the number is most wanted for.
// Returns nothing when the image has too few spots to have a fall-off at all.
std::optional<float> GetResolution(const std::vector<SpotToSave> &spots);

void SpotAnalyze(const DiffractionExperiment &experiment,
                 const SpotFindingSettings &settings,
                 const std::vector<DiffractionSpot> &spots,
                 DataMessage &message);