Files
Jungfraujoch/image_analysis/geom_refinement/GeometryRefiner.cpp
T
leonarski_fandClaude Opus 5.5 ae7b68dd68 rugnux stills: a given cell is where the geometry refinement starts, not what it fits the distance to
On stills a cell and a detector distance are degenerate: a spot's radius fixes only their ratio. The
geometry refinement that -C switches on anchored the cell and refined the distance, so a deposited cell
a percent off this crystal moved a correct distance by as much (MPCCD: 50.47 -> 50.14 mm, R-free
0.259 -> 0.318). Now the distance is held and the cell refined from the spots, starting from the given
one. Only where the frames have rejected the file's distance (DecideStillsGeometry's grid, which is what
-C recovers a bad header distance with) is the cell anchored and the distance refined from it. The grid
itself asks the given cell, not one refined at the file's distance.

Co-Authored-By: Claude Opus 5.5 <noreply@anthropic.com>
2026-10-20 16:39:44 +02:00

323 lines
16 KiB
C++

// SPDX-FileCopyrightText: 2026 Filip Leonarski, Paul Scherrer Institute <filip.leonarski@psi.ch>
// SPDX-License-Identifier: GPL-3.0-only
#include "GeometryRefiner.h"
#include <algorithm>
#include <array>
#include <cmath>
#include <vector>
#include "../../common/JFJochMath.h" // PI
#include "LatticeReduction.h"
#include "XtalResidual.h"
#include "ceres/ceres.h"
namespace {
// Trigonal is described with the hexagonal cell + B, same as the per-image XtalOptimizer.
gemmi::CrystalSystem MapSystem(gemmi::CrystalSystem s) {
return (s == gemmi::CrystalSystem::Trigonal) ? gemmi::CrystalSystem::Hexagonal : s;
}
// The cell angles (radians) that XtalResidual bakes into its B matrix for a given system. Only
// monoclinic (beta) and triclinic (all three) read p2; the rest use fixed symmetry angles. We keep the
// angles constant in v1, so these are set once from the input cell.
void InitCellAngles(gemmi::CrystalSystem system, const UnitCell &cell, double ang[3]) {
const double d2r = PI / 180.0;
switch (system) {
case gemmi::CrystalSystem::Hexagonal:
ang[0] = PI / 2.0; ang[1] = PI / 2.0; ang[2] = 2.0 * PI / 3.0;
break;
case gemmi::CrystalSystem::Monoclinic:
// XtalResidual reads p2[0] as beta.
ang[0] = cell.beta * d2r; ang[1] = PI / 2.0; ang[2] = PI / 2.0;
break;
case gemmi::CrystalSystem::Triclinic:
ang[0] = cell.alpha * d2r; ang[1] = cell.beta * d2r; ang[2] = cell.gamma * d2r;
break;
default: // orthorhombic / tetragonal / cubic
ang[0] = PI / 2.0; ang[1] = PI / 2.0; ang[2] = PI / 2.0;
break;
}
}
// Effective (lengths, alpha,beta,gamma) that reproduce the lattice XtalResidual builds from (len, ang),
// so a frame's lattice can be reconstructed with AngleAxisAndCellToLattice for HKL re-assignment.
void EffectiveCell(gemmi::CrystalSystem system, const double len[3], const double ang[3],
double lengths[3], double &alpha, double &beta, double &gamma) {
switch (system) {
case gemmi::CrystalSystem::Hexagonal:
lengths[0] = len[0]; lengths[1] = len[0]; lengths[2] = len[2];
alpha = PI / 2.0; beta = PI / 2.0; gamma = 2.0 * PI / 3.0;
break;
case gemmi::CrystalSystem::Tetragonal:
lengths[0] = len[0]; lengths[1] = len[0]; lengths[2] = len[2];
alpha = PI / 2.0; beta = PI / 2.0; gamma = PI / 2.0;
break;
case gemmi::CrystalSystem::Cubic:
lengths[0] = len[0]; lengths[1] = len[0]; lengths[2] = len[0];
alpha = PI / 2.0; beta = PI / 2.0; gamma = PI / 2.0;
break;
case gemmi::CrystalSystem::Monoclinic:
lengths[0] = len[0]; lengths[1] = len[1]; lengths[2] = len[2];
alpha = PI / 2.0; beta = ang[0]; gamma = PI / 2.0;
break;
case gemmi::CrystalSystem::Triclinic:
lengths[0] = len[0]; lengths[1] = len[1]; lengths[2] = len[2];
alpha = ang[0]; beta = ang[1]; gamma = ang[2];
break;
default: // orthorhombic
lengths[0] = len[0]; lengths[1] = len[1]; lengths[2] = len[2];
alpha = PI / 2.0; beta = PI / 2.0; gamma = PI / 2.0;
break;
}
}
// Orientation seed (angle-axis) for a frame's lattice, using the per-system decomposition the per-image
// optimizer uses so it matches XtalResidual's B convention.
void OrientationSeed(gemmi::CrystalSystem system, const CrystalLattice &latt, double rod[3]) {
double scratch[3];
if (system == gemmi::CrystalSystem::Hexagonal) {
LatticeToRodriguesAndLengths_Hex(latt, rod, scratch);
} else if (system == gemmi::CrystalSystem::Monoclinic) {
double beta;
LatticeToRodriguesLengthsBeta_Mono(latt, rod, scratch, beta);
} else {
LatticeToRodriguesAndLengths_GS(latt, rod, scratch);
}
}
UnitCell BuildUnitCell(gemmi::CrystalSystem system, const double len[3], const double ang[3]) {
const double r2d = 180.0 / PI;
UnitCell uc{};
switch (system) {
case gemmi::CrystalSystem::Hexagonal:
uc = {(float)len[0], (float)len[0], (float)len[2], 90.0f, 90.0f, 120.0f};
break;
case gemmi::CrystalSystem::Tetragonal:
uc = {(float)len[0], (float)len[0], (float)len[2], 90.0f, 90.0f, 90.0f};
break;
case gemmi::CrystalSystem::Cubic:
uc = {(float)len[0], (float)len[0], (float)len[0], 90.0f, 90.0f, 90.0f};
break;
case gemmi::CrystalSystem::Monoclinic:
uc = {(float)len[0], (float)len[1], (float)len[2], 90.0f, (float)(ang[0] * r2d), 90.0f};
break;
case gemmi::CrystalSystem::Triclinic:
uc = {(float)len[0], (float)len[1], (float)len[2],
(float)(ang[0] * r2d), (float)(ang[1] * r2d), (float)(ang[2] * r2d)};
break;
default: // orthorhombic
uc = {(float)len[0], (float)len[1], (float)len[2], 90.0f, 90.0f, 90.0f};
break;
}
return uc;
}
// Anchors the cell lengths to the input cell. Penalises each length's deviation from its input value
// with a large weight, breaking the low-resolution distance<->cell-scale degeneracy (position ~
// distance / cell_scale) so distance is determined by the data with the cell pinned.
struct CellLengthRegularizer {
double w0, w1, w2;
double l0, l1, l2;
template <typename T>
bool operator()(const T *const len, T *r) const {
r[0] = T(w0) * (len[0] - T(l0));
r[1] = T(w1) * (len[1] - T(l1));
r[2] = T(w2) * (len[2] - T(l2));
return true;
}
};
} // namespace
GeometryRefinerResult RefineGlobalGeometry(const DiffractionGeometry &nominal_geom,
const UnitCell &input_cell,
const std::vector<GeomRefineFrame> &frames,
const GeometryRefinerSettings &settings) {
GeometryRefinerResult result;
try {
const gemmi::CrystalSystem system = MapSystem(settings.crystal_system);
// Shared geometry parameter blocks (refined). Detector tilt and the rotation axis are constant.
double beam[2] = {nominal_geom.GetBeamX_pxl(), nominal_geom.GetBeamY_pxl()};
double distance_mm = nominal_geom.GetDetectorDistance_mm();
double detector_rot[2] = {nominal_geom.GetPoniRot1_rad(), nominal_geom.GetPoniRot2_rad()};
double rot_vec[3] = {1.0, 0.0, 0.0};
const double rot3 = nominal_geom.GetPoniRot3_rad();
// Same for every spot of every frame, so taken once here rather than per residual.
const double cos_rot3 = std::cos(rot3), sin_rot3 = std::sin(rot3);
const DetectorOrientation orientation = nominal_geom.GetOrientation();
const double lambda = nominal_geom.GetWavelength_A();
const double pixel = nominal_geom.GetPixelSize_mm();
// Shared cell blocks. Lengths refined (regularized); angles constant.
double cell_len[3] = {input_cell.a, input_cell.b, input_cell.c};
const double cell_len0[3] = {input_cell.a, input_cell.b, input_cell.c};
double cell_ang[3];
InitCellAngles(system, input_cell, cell_ang);
double eff_len[3], eff_alpha, eff_beta, eff_gamma; // recomputed each round from cell_len/ang
// Per-frame orientation seeds.
std::vector<std::array<double, 3>> orient(frames.size());
for (size_t i = 0; i < frames.size(); ++i)
OrientationSeed(system, frames[i].lattice, orient[i].data());
// Reciprocal length of one detector pixel at the nominal geometry, used to scale the robust
// loss (~3 px) into the reciprocal-space residual units.
const double recip_per_px = pixel / (distance_mm * lambda);
const double loss_scale = 3.0 * recip_per_px;
// Tolerance schedule (fractional-hkl norm), tightening each round like the per-image optimizer.
auto round_tol = [&](int r) {
if (settings.rounds <= 1) return 0.2;
const double t = static_cast<double>(r) / (settings.rounds - 1);
return 0.3 - (0.3 - 0.1) * t;
};
// Whether the last solve that ran produced a usable solution; folded into result.ok below,
// which otherwise reports success on spot and frame counts alone.
bool solve_usable = false;
for (int round = 0; round < settings.rounds; ++round) {
EffectiveCell(system, cell_len, cell_ang, eff_len, eff_alpha, eff_beta, eff_gamma);
DiffractionGeometry cur = nominal_geom;
cur.BeamX_pxl(beam[0]).BeamY_pxl(beam[1]).DetectorDistance_mm(distance_mm);
const double tol = round_tol(round);
const double tol_sq = tol * tol;
ceres::Problem problem;
auto ordering = std::make_shared<ceres::ParameterBlockOrdering>();
int spots_used = 0, frames_used = 0;
for (size_t i = 0; i < frames.size(); ++i) {
const CrystalLattice latt = AngleAxisAndCellToLattice(
orient[i].data(), eff_len, eff_alpha, eff_beta, eff_gamma);
const Coord v0 = latt.Vec0(), v1 = latt.Vec1(), v2 = latt.Vec2();
int used_in_frame = 0;
for (const auto &s : frames[i].spots) {
const Coord recip = cur.DetectorToRecip(s.x, s.y);
const double hf = recip * v0, kf = recip * v1, lf = recip * v2;
const double h = std::round(hf), k = std::round(kf), l = std::round(lf);
const double dn = (hf - h) * (hf - h) + (kf - k) * (kf - k) + (lf - l) * (lf - l);
if (dn > tol_sq)
continue;
problem.AddResidualBlock(
new ceres::AutoDiffCostFunction<XtalResidual, 3, 2, 1, 2, 3, 3, 3, 3>(
new XtalResidual(s.x, s.y, lambda, pixel, cos_rot3, sin_rot3, 0.0,
h, k, l, system, orientation)),
new ceres::CauchyLoss(loss_scale),
beam, &distance_mm, detector_rot, rot_vec, orient[i].data(), cell_len, cell_ang);
++used_in_frame;
++spots_used;
}
if (used_in_frame > 0) {
ordering->AddElementToGroup(orient[i].data(), 0); // eliminate orientations first
++frames_used;
}
}
if (spots_used < settings.min_spots_total) {
if (round == 0)
return result; // ok stays false
break; // keep the previous round's solution
}
// Cell-length regularizer (weight ~ coeff * sqrt(N_obs) / L0^2 -> effectively pins the cell).
const double sqrtN = std::sqrt(static_cast<double>(spots_used));
CellLengthRegularizer *reg = new CellLengthRegularizer{
settings.cell_reg_coeff * sqrtN / (cell_len0[0] * cell_len0[0]),
settings.cell_reg_coeff * sqrtN / (cell_len0[1] * cell_len0[1]),
settings.cell_reg_coeff * sqrtN / (cell_len0[2] * cell_len0[2]),
cell_len0[0], cell_len0[1], cell_len0[2]};
problem.AddResidualBlock(
new ceres::AutoDiffCostFunction<CellLengthRegularizer, 3, 3>(reg), nullptr, cell_len);
// Shared blocks go in the second elimination group; constant ones are stripped by Ceres.
for (double *b : {beam, &distance_mm, detector_rot, rot_vec, cell_len, cell_ang})
ordering->AddElementToGroup(b, 1);
// Beam + distance bounds around the nominal value; cell lengths loosely bounded (the
// regularizer does the anchoring).
problem.SetParameterLowerBound(beam, 0, nominal_geom.GetBeamX_pxl() - settings.beam_range_px);
problem.SetParameterUpperBound(beam, 0, nominal_geom.GetBeamX_pxl() + settings.beam_range_px);
problem.SetParameterLowerBound(beam, 1, nominal_geom.GetBeamY_pxl() - settings.beam_range_px);
problem.SetParameterUpperBound(beam, 1, nominal_geom.GetBeamY_pxl() + settings.beam_range_px);
problem.SetParameterLowerBound(&distance_mm, 0,
std::max(1.0, nominal_geom.GetDetectorDistance_mm() - settings.distance_range_mm));
problem.SetParameterUpperBound(&distance_mm, 0,
nominal_geom.GetDetectorDistance_mm() + settings.distance_range_mm);
for (int j = 0; j < 3; ++j) {
problem.SetParameterLowerBound(cell_len, j, 0.7 * cell_len0[j]);
problem.SetParameterUpperBound(cell_len, j, 1.3 * cell_len0[j]);
}
if (!settings.refine_distance)
problem.SetParameterBlockConstant(&distance_mm);
problem.SetParameterBlockConstant(detector_rot); // tilt not refined
problem.SetParameterBlockConstant(rot_vec);
problem.SetParameterBlockConstant(cell_ang); // angles not refined in v1
ceres::Solver::Options options;
options.linear_solver_type = ceres::DENSE_SCHUR;
options.linear_solver_ordering = ordering;
options.num_threads = std::max(1, settings.num_threads);
options.max_num_iterations = 100;
options.max_solver_time_in_seconds = 60.0;
options.logging_type = ceres::LoggingType::SILENT;
options.minimizer_progress_to_stdout = false;
ceres::Solver::Summary summary;
ceres::Solve(options, &problem, &summary);
solve_usable = summary.IsSolutionUsable();
result.frames_used = frames_used;
result.spots_used = spots_used;
}
// Final fit quality: median detector residual of the retained spots at the refined geometry.
EffectiveCell(system, cell_len, cell_ang, eff_len, eff_alpha, eff_beta, eff_gamma);
DiffractionGeometry cur = nominal_geom;
cur.BeamX_pxl(beam[0]).BeamY_pxl(beam[1]).DetectorDistance_mm(distance_mm);
std::vector<double> residuals;
for (size_t i = 0; i < frames.size(); ++i) {
const CrystalLattice latt = AngleAxisAndCellToLattice(
orient[i].data(), eff_len, eff_alpha, eff_beta, eff_gamma);
const Coord a = latt.Astar(), b = latt.Bstar(), c = latt.Cstar();
const Coord v0 = latt.Vec0(), v1 = latt.Vec1(), v2 = latt.Vec2();
for (const auto &s : frames[i].spots) {
const Coord recip = cur.DetectorToRecip(s.x, s.y);
const double hf = recip * v0, kf = recip * v1, lf = recip * v2;
const double h = std::round(hf), k = std::round(kf), l = std::round(lf);
const double dn = (hf - h) * (hf - h) + (kf - k) * (kf - k) + (lf - l) * (lf - l);
if (dn > 0.1 * 0.1)
continue;
const Coord recip_pred = a * (float)h + b * (float)k + c * (float)l;
const auto [px, py] = cur.RecipToDetector(recip_pred);
if (std::isfinite(px) && std::isfinite(py))
residuals.push_back(std::hypot(px - s.x, py - s.y));
}
}
if (!residuals.empty()) {
std::nth_element(residuals.begin(), residuals.begin() + residuals.size() / 2, residuals.end());
result.median_residual_px = residuals[residuals.size() / 2];
}
result.ok = solve_usable && result.spots_used >= settings.min_spots_total && result.frames_used > 0;
result.beam_x_px = beam[0];
result.beam_y_px = beam[1];
result.distance_mm = distance_mm;
result.cell = BuildUnitCell(system, cell_len, cell_ang);
return result;
} catch (...) {
result.ok = false;
return result;
}
}