A crystal in the corpus was reported as two because the grid point joining its halves scored 0.498 - two thousandths under the threshold. That is an artefact of putting a hard edge through a continuous quantity, not a gap in a crystal. The patch search is now hysteresis. A patch is labelled at a lower grow threshold (0.35) and kept only if it holds a cell above the seed threshold (0.50), which is the same thing as growing out of the seeds in one pass of the labeller rather than two. A cell between the two levels joins a crystal that already exists but can never start one, so no lowering of the grow threshold can turn a background into a crystal - and the negatives are safe by construction, since water peaks at 0.146 and ice at 0.490, both under the seed level. Both halves of the small-patch rule read the GROWN patch - the count includes the cells growth added and the peak is the patch's best cell wherever it lies - which is stated at the test, because a reader will otherwise wonder whether a grown cell can rescue a patch no seed would have admitted. It cannot: the patch is discarded before that test unless it holds a seed. The reported extents are those of the grown patch, so they reach the 0.35 contour. Over the corpus that is major_um x1.04 and n_images x1.07 at the median (x1.11 and x1.14 at the mean, +7% cells overall), and the cells it adds are spread fairly evenly over 0.35-0.50 rather than piled at the bottom - a crystal edge sampled at one grid step, not bleed into a neighbour that never diffracted. The patch mean falls with them, and can now sit below the seed threshold; the peak beside it is what the admission was decided on. RASTER_REPORT_VERSION is 3, because N_CELLS and the extents are a different measurement under the same names. The corpus table is unchanged: 17/17 protein, 0/4 water, 0/3 ice, 10/10 heldout. The split heals into one crystal, and one raster's five patches become three. Co-Authored-By: Claude Opus 5 <noreply@anthropic.com> Claude-Session: https://claude.ai/code/session_01EFEJG6WBQv8th4UJFNe53N
237 lines
11 KiB
C++
237 lines
11 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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#include <algorithm>
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#include <cmath>
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#include <utility>
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#include "../../common/ConnectedComponents.h"
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#include "../../common/JFJochMath.h"
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#include "AnalyzeGridScan.h"
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namespace {
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constexpr float NO_VALUE = -1.0f;
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}
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GridScanResult AnalyzeGridScan(const ScanResult &scan,
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const GridScanSettings &grid,
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float beam_size_x_um,
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float beam_size_y_um,
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const GridScanAnalysisParameters ¶ms) {
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const int64_t nx = grid.GetGridSizeX_step();
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const int64_t ny = grid.GetGridSizeY_step();
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const float step_x = fabsf(grid.GetGridStepX_um());
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const float step_y = fabsf(grid.GetGridStepY_um());
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// Scatter the per-image quantities onto the display grid. Rearrange knows about snake order,
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// the vertical flag and the step signs, so nothing here has to.
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std::vector<float> protein(nx * ny, NO_VALUE);
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std::vector<float> ice(nx * ny, NO_VALUE);
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std::vector<float> res(nx * ny, NO_VALUE);
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std::vector<int64_t> image_no(nx * ny, -1);
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for (const auto &elem: scan.images) {
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if (elem.number < 0 || elem.number >= grid.GetNElem())
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continue;
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const int64_t i = grid.Rearrange(elem.number);
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protein[i] = elem.protein_score.value_or(NO_VALUE);
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ice[i] = elem.ice_score.value_or(NO_VALUE);
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res[i] = elem.res.value_or(NO_VALUE);
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image_no[i] = elem.number;
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}
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// Hysteresis. The patches are labelled at the GROW level and then only those holding at least
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// one cell at the SEED level are kept, which is the same thing as growing out of the seeds and
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// is one pass of the labeller rather than two. A cell between the two levels therefore joins a
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// crystal that already exists but can never start one, so however low the grow level is set, a
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// background that never reaches the seed level produces nothing.
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std::vector<uint8_t> grown(nx * ny);
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for (int64_t i = 0; i < nx * ny; i++)
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grown[i] = (protein[i] > params.grow_score_threshold) ? 1 : 0;
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// Labelled with no size cut of its own: whether a patch is big enough is no longer a plain
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// floor - a small patch survives on the strength of its diffraction - and that test needs the
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// patch's scores, which the labeller does not have.
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const std::vector<int32_t> label = LabelConnectedComponents(grown, nx, ny, 1);
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const int32_t n_label = label.empty() ? 0 : *std::max_element(label.begin(), label.end());
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GridScanResult result;
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result.beam_size_x_um = beam_size_x_um;
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result.beam_size_y_um = beam_size_y_um;
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for (int32_t l = 1; l <= n_label; l++) {
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std::vector<int64_t> cell;
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for (int64_t i = 0; i < nx * ny; i++) {
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if (label[i] == l)
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cell.push_back(i);
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}
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if (cell.empty())
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continue;
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// Hysteresis, the second half: a patch that never reaches the seed level is not a patch,
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// whatever its shape, so nothing about it is worth measuring.
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bool has_seed = false;
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for (int64_t i: cell)
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has_seed = has_seed || protein[i] > params.protein_score_threshold;
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if (!has_seed)
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continue;
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const auto n = static_cast<float>(cell.size());
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// Cell centres in MICROMETRES, taken once. Every geometric quantity below is computed from
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// these and never from cell units: step_x and step_y genuinely differ (20 x 16 um is an
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// ordinary raster), so a second moment taken in cells gives the wrong axis angle.
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// The i / nx and i % nx are the row and column of a row-major index - an index split, and
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// truncation is the whole point of it; there is no precision to lose there.
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std::vector<float> px(cell.size()), py(cell.size());
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for (size_t k = 0; k < cell.size(); k++) {
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px[k] = static_cast<float>(cell[k] % nx) * step_x;
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py[k] = static_cast<float>(cell[k] / nx) * step_y;
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}
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// Centre, pulled towards the cells that diffract best. The pull uses the RANK of the
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// resolution within the blob, never its value: the best cell gets p = 1, the worst p = 0,
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// and a cell with no resolution at all gets p = 0 rather than being dropped. A salt grain
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// reporting an absurd 0.8 A is then weighted exactly like a genuine best cell, so no
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// artefact can drag the centre however extreme its number is.
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std::vector<int64_t> by_res;
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for (int64_t i: cell) {
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if (res[i] > 0)
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by_res.push_back(i);
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}
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std::sort(by_res.begin(), by_res.end(), [&](int64_t a, int64_t b) { return res[a] < res[b]; });
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std::vector<float> weight(cell.size(), 1.0f);
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for (size_t r = 0; r < by_res.size(); r++) {
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const float p = (by_res.size() == 1) ? 1.0f
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: 1.0f - static_cast<float>(r) / static_cast<float>(by_res.size() - 1);
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// cell is built in ascending grid order, so it can be searched directly
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weight[std::lower_bound(cell.begin(), cell.end(), by_res[r]) - cell.begin()] = 1.0f + 0.5f * p;
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}
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float sum_w = 0, sum_wx = 0, sum_wy = 0;
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for (size_t k = 0; k < cell.size(); k++) {
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sum_w += weight[k];
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sum_wx += weight[k] * px[k];
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sum_wy += weight[k] * py[k];
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}
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const float cx_um = sum_wx / sum_w;
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const float cy_um = sum_wy / sum_w;
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// A weighted centroid of a banana- or L-shaped blob can land outside the blob, where no
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// image was ever collected. The image number has to name a cell that exists, so snap.
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size_t nearest = 0;
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float nearest_d2 = INFINITY;
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for (size_t k = 0; k < cell.size(); k++) {
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const float d2 = (px[k] - cx_um) * (px[k] - cx_um) + (py[k] - cy_um) * (py[k] - cy_um);
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if (d2 < nearest_d2) {
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nearest_d2 = d2;
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nearest = k;
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}
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}
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float sxx = 0, syy = 0, sxy = 0;
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for (size_t k = 0; k < cell.size(); k++) {
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const float dx = px[k] - cx_um;
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const float dy = py[k] - cy_um;
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sxx += dx * dx;
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syy += dy * dy;
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sxy += dx * dy;
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}
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const float angle = 0.5f * atan2f(2 * sxy, sxx - syy);
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const float cos_a = cosf(angle);
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const float sin_a = sinf(angle);
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// Direction from the eigenvector, LENGTH from the projected extent. "How far do I scan"
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// is an extent question, and the constant taking a second moment to a length depends on
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// an assumed shape that a blob of a few cells does not have.
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float min_u = INFINITY, max_u = -INFINITY, min_v = INFINITY, max_v = -INFINITY;
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for (size_t k = 0; k < cell.size(); k++) {
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const float dx = px[k] - cx_um;
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const float dy = py[k] - cy_um;
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min_u = std::min(min_u, dx * cos_a + dy * sin_a);
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max_u = std::max(max_u, dx * cos_a + dy * sin_a);
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min_v = std::min(min_v, -dx * sin_a + dy * cos_a);
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max_v = std::max(max_v, -dx * sin_a + dy * cos_a);
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}
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// The span runs between cell centres, so one cell has to be added back. A cell is a
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// step_x by step_y rectangle, and its own width along a direction is that rectangle's
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// support width - which is the plain step only when the axis lies along the grid.
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const float cell_along_u = fabsf(step_x * cos_a) + fabsf(step_y * sin_a);
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const float cell_along_v = fabsf(step_x * sin_a) + fabsf(step_y * cos_a);
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float sum_protein = 0, sum_ice = 0, peak_protein = 0;
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for (int64_t i: cell) {
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sum_protein += protein[i];
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sum_ice += std::max(ice[i], 0.0f);
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peak_protein = std::max(peak_protein, protein[i]);
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}
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// A patch is a crystal when it is big enough to be a shape rather than a coincidence, OR
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// when it is smaller than that but the diffraction in it is decisive on its own. One cell
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// is enough where that cell is clearly protein; a weak patch still has to be a shape.
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//
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// Both halves are read over the GROWN patch: the count includes the cells hysteresis added
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// and the peak is the patch's best cell wherever it lies. That cannot let growth rescue a
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// patch no seed would have admitted, because the patch has already been discarded above
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// unless it holds a seed cell - and a seed cell is by definition the strongest kind there
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// is, so the peak of a grown patch is the peak of its seeds.
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if (static_cast<int64_t>(cell.size()) < params.min_blob_cells
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&& peak_protein < params.decisive_protein_score)
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continue;
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GridScanCrystal crystal;
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crystal.nx = cx_um / step_x;
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crystal.ny = cy_um / step_y;
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crystal.x_um = cx_um;
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crystal.y_um = cy_um;
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crystal.image_number = image_no[cell[nearest]];
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crystal.major_um = max_u - min_u + cell_along_u;
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crystal.minor_um = max_v - min_v + cell_along_v;
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crystal.angle_deg = angle * 180.0f / static_cast<float>(PI);
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// The angle is the axis of the larger second MOMENT, the extents are MEASURED spans, and
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// for a strongly non-convex blob the two can disagree about which axis is the longer.
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// A consumer draws a major by minor frame rotated by angle_deg, so keep both facts by
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// turning the frame a quarter turn rather than by dropping one of them.
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if (crystal.major_um < crystal.minor_um) {
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std::swap(crystal.major_um, crystal.minor_um);
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crystal.angle_deg += 90.0f;
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}
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// atan2 returns (-pi,pi], so the half-angle is in (-pi/2,pi/2] and the quarter turn above
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// can carry it past 180; an axis has no sign, so fold it into [0,180).
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if (crystal.angle_deg < 0)
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crystal.angle_deg += 180.0f;
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if (crystal.angle_deg >= 180.0f)
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crystal.angle_deg -= 180.0f;
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// The MEAN protein score, not the peak: the score saturates, so the peak is 1.0 for every
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// real crystal and ranks nothing. The mean stays a detection confidence and compares.
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crystal.score = sum_protein / n;
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crystal.ice_score = sum_ice / n;
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crystal.peak_score = peak_protein;
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// The 25th percentile, not the minimum: the single best cell in a blob is precisely where
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// a salt spot or a hot pixel shows up.
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if (!by_res.empty()) {
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const auto q = static_cast<size_t>(0.25 * static_cast<double>(by_res.size() - 1) + 0.5);
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crystal.res_A = res[by_res[q]];
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}
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crystal.n_images = static_cast<int64_t>(cell.size());
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result.crystals.push_back(crystal);
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}
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std::sort(result.crystals.begin(), result.crystals.end(),
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[](const GridScanCrystal &a, const GridScanCrystal &b) { return a.score > b.score; });
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// Kept to the best few only where a caller asked for that; the sort above is what makes the
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// ones it keeps the right ones.
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if (params.max_crystals > 0
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&& result.crystals.size() > static_cast<size_t>(params.max_crystals))
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result.crystals.resize(params.max_crystals);
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return result;
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}
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