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This is an UNSTABLE release. This version adds scalign and merging. These are experimental at the moment, and should not be used for production analysis. If things go wrong with analysis, it is better to revert to 1.0.0-rc.124. * jfjoch_broker: Improve logic on switching on/off spot finding * jfjoch_broker: Increase maximum spot count for FFBIDX to 65536 * jfjoch_broker: Increase default maximum unit cell for FFT to 500 A (could have performance impact, TBD) * jfjoch_process: Add scalign and merging functionality - program is experimental at the moment and should not be used for production analysis * jfjoch_viewer: Display partiality and reciprocal Lorentz-polarization correction for each reflection * jfjoch_writer: Save more information about each reflection Reviewed-on: #32 Co-authored-by: Filip Leonarski <filip.leonarski@psi.ch> Co-committed-by: Filip Leonarski <filip.leonarski@psi.ch>
645 lines
23 KiB
C++
645 lines
23 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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#include "XtalOptimizer.h"
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#include "ceres/ceres.h"
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#include "ceres/rotation.h"
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struct XtalResidual {
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XtalResidual(double x, double y,
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double lambda,
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double pixel_size,
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double angle_rad,
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double exp_h, double exp_k,
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double exp_l,
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gemmi::CrystalSystem symmetry)
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: obs_x(x), obs_y(y),
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lambda(lambda),
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pixel_size(pixel_size),
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exp_h(exp_h),
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exp_k(exp_k),
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exp_l(exp_l),
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angle_rad(angle_rad),
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symmetry(symmetry) {
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}
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template<typename T>
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bool operator()(const T *const beam_x,
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const T *const beam_y,
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const T *const distance_mm,
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const T *const detector_rot,
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const T *const rotation_axis,
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const T *const p0,
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const T *const p1,
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const T *const p2,
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T *residual) const {
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// PyFAI convention (left-handed for rot1/rot2):
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// poni_rot = Rz(-rot3) * Rx(-rot2) * Ry(+rot1)
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// detector_rot[0] = rot1, detector_rot[1] = rot2 (rot3 = 0 assumed)
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const T rot1 = detector_rot[0];
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const T rot2 = detector_rot[1];
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// Ry(+rot1): rotation around Y-axis
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const T c1 = ceres::cos(rot1);
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const T s1 = ceres::sin(rot1);
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// Rx(-rot2): rotation around X-axis with inverted sign (PyFAI left-handed)
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const T c2 = ceres::cos(-rot2);
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const T s2 = ceres::sin(-rot2);
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// Detector coordinates in mm
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T det_x = (T(obs_x) - beam_x[0]) * T(pixel_size);
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T det_y = (T(obs_y) - beam_y[0]) * T(pixel_size);
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T det_z = T(distance_mm[0]);
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// Apply Ry(rot1) first: rotate around Y
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T t1_x = c1 * det_x + s1 * det_z;
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T t1_y = det_y;
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T t1_z = -s1 * det_x + c1 * det_z;
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// Then apply Rx(-rot2): rotate around X
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T x = t1_x;
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T y = c2 * t1_y - s2 * t1_z;
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T z = s2 * t1_y + c2 * t1_z;
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// convert to recip space
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T lab_norm = ceres::sqrt(x * x + y * y + z * z);
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T recip[3];
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recip[0] = x / (lab_norm * T(lambda));
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recip[1] = y / (lab_norm * T(lambda));
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recip[2] = (z / lab_norm - T(1.0)) / T(lambda);
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Eigen::Map<const Eigen::Matrix<T, 3, 1>> e_obs_recip_raw(recip);
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// Apply goniometer "back-to-start" rotation:
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// brings observed reciprocal from image orientation into reference crystal frame
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T v[3], rot_arr[9];
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v[0] = T(angle_rad) * rotation_axis[0];
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v[1] = T(angle_rad) * rotation_axis[1];
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v[2] = T(angle_rad) * rotation_axis[2];
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ceres::AngleAxisToRotationMatrix(v, rot_arr);
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Eigen::Matrix<T, 3, 3> R_gonio_back(rot_arr);
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Eigen::Matrix<T, 3, 1> e_obs_recip = R_gonio_back * e_obs_recip_raw;
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Eigen::Matrix<T, 3, 1> e_pred;
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Eigen::Matrix<T, 3, 3> e_latt;
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T uc_rot_matrix[9];
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ceres::AngleAxisToRotationMatrix(p0, uc_rot_matrix);
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Eigen::Map<const Eigen::Matrix<T, 3, 3>> e_uc_rot_matrix(uc_rot_matrix);
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Eigen::Matrix<T, 3, 1> e_uc_len = Eigen::Matrix<T, 3, 1>::Zero();
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Eigen::Matrix<T, 3, 3> B = Eigen::Matrix<T, 3, 3>::Identity();
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if (symmetry == gemmi::CrystalSystem::Hexagonal) {
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e_uc_len << p1[0], p1[0], p1[2];
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B(0, 1) = T(-0.5); // cos(120)
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B(1, 1) = T(sqrt(3.0) / 2.0); // sin(120)
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} else if (symmetry == gemmi::CrystalSystem::Orthorhombic) {
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e_uc_len << p1[0], p1[1], p1[2];
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} else if (symmetry == gemmi::CrystalSystem::Tetragonal) {
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e_uc_len << p1[0], p1[0], p1[2];
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} else if (symmetry == gemmi::CrystalSystem::Cubic) {
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e_uc_len << p1[0], p1[0], p1[0];
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} else if (symmetry == gemmi::CrystalSystem::Monoclinic) {
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// Unique axis b: alpha = gamma = 90°, beta free (angle between a and c)
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e_uc_len << p1[0], p1[1], p1[2];
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B(0, 2) = ceres::cos(p2[0]);
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B(2, 2) = ceres::sin(p2[0]);
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} else {
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// Triclinic: p1 = (a,b,c), p2 = (alpha, beta, gamma) in radians
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const T ca = ceres::cos(p2[0]);
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const T cb = ceres::cos(p2[1]);
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const T cg = ceres::cos(p2[2]);
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const T sg = ceres::sin(p2[2]);
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e_uc_len << p1[0], p1[1], p1[2];
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// B_triclinic builds lattice from lengths+angles in crystallographic convention
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// columns correspond to a, b, c in Cartesian frame prior to global rotation
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B(0, 0) = T(1);
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B(1, 0) = T(0);
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B(2, 0) = T(0);
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B(0, 1) = cg;
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B(1, 1) = sg;
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B(2, 1) = T(0);
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// c vector components:
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T cx = cb;
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T cy = (ca - cb * cg) / sg;
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T v = T(1) - cx * cx - cy * cy;
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T cz;
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if (v >= T(0))
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cz = ceres::sqrt(v);
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else
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cz = T(0);
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B(0, 2) = cx;
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B(1, 2) = cy;
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B(2, 2) = cz;
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}
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e_latt = e_uc_rot_matrix * e_uc_len.asDiagonal() * B;
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Eigen::Matrix<T, 3, 1> e_hkl;
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e_hkl << T(exp_h), T(exp_k), T(exp_l);
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auto e_pred_hkl = e_latt.transpose() * e_obs_recip;
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residual[0] = exp_h - e_pred_hkl[0];
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residual[1] = exp_k - e_pred_hkl[1];
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residual[2] = exp_l - e_pred_hkl[2];
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return true;
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}
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const double obs_x, obs_y;
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const double lambda;
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const double pixel_size;
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const double exp_h;
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const double exp_k;
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const double exp_l;
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const double angle_rad;
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gemmi::CrystalSystem symmetry;
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};
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inline void LatticeToRodriguesAndLengths_GS(const CrystalLattice &latt,
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double rod[3],
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double lengths[3]) {
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// Load lattice columns
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const Coord a = latt.Vec0();
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const Coord b = latt.Vec1();
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const Coord c = latt.Vec2();
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Eigen::Vector3d A(a[0], a[1], a[2]);
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Eigen::Vector3d B(b[0], b[1], b[2]);
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Eigen::Vector3d C(c[0], c[1], c[2]);
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// Lengths = column norms (orthorhombic assumption)
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lengths[0] = A.norm();
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lengths[1] = B.norm();
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lengths[2] = C.norm();
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auto safe_unit = [](const Eigen::Vector3d &v, double eps = 1e-15) -> Eigen::Vector3d {
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double n = v.norm();
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return (n > eps) ? (v / n) : Eigen::Vector3d(1.0, 0.0, 0.0);
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};
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// Gram–Schmidt with original order: x from A, y from B orthogonalized vs x
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Eigen::Vector3d e1 = safe_unit(A);
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Eigen::Vector3d y = B - (e1.dot(B)) * e1;
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Eigen::Vector3d e2 = safe_unit(y);
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// z from cross to ensure right-handed basis
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Eigen::Vector3d e3 = e1.cross(e2);
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double n3 = e3.norm();
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if (n3 < 1e-15) {
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// Degenerate case: B nearly collinear with A → use C instead
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y = C - (e1.dot(C)) * e1;
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e2 = safe_unit(y);
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e3 = e1.cross(e2);
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n3 = e3.norm();
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if (n3 < 1e-15) {
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// Still degenerate: pick any perpendicular to e1
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e2 = safe_unit((std::abs(e1.x()) < 0.9)
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? Eigen::Vector3d::UnitX().cross(e1)
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: Eigen::Vector3d::UnitY().cross(e1));
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e3 = e1.cross(e2);
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}
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} else {
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e3 /= n3;
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}
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Eigen::Matrix3d R;
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R.col(0) = e1;
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R.col(1) = e2;
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R.col(2) = e3;
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// Convert rotation to Rodrigues (axis * angle)
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Eigen::AngleAxisd aa(R);
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Eigen::Vector3d r = aa.angle() * aa.axis();
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rod[0] = r.x();
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rod[1] = r.y();
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rod[2] = r.z();
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}
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void LatticeToRodriguesAndLengths_Hex(const CrystalLattice &latt, double rod[3], double ac[3]) {
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const Coord a = latt.Vec0();
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const Coord b = latt.Vec1();
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const Coord c = latt.Vec2();
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Eigen::Vector3d A(a[0], a[1], a[2]);
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Eigen::Vector3d B(b[0], b[1], b[2]);
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Eigen::Vector3d C(c[0], c[1], c[2]);
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const double a_len = A.norm();
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const double b_len = B.norm();
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const double c_len = C.norm();
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ac[0] = (a_len + b_len) / 2.0;
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ac[1] = (a_len + b_len) / 2.0;
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ac[2] = c_len;
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Eigen::Vector3d e1;
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Eigen::Vector3d e3;
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if (a_len > 0.0)
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e1 = A / a_len;
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else
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e1 = Eigen::Vector3d::UnitX();
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if (c_len > 0.0)
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e3 = C / c_len;
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else
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e3 = Eigen::Vector3d::UnitZ();
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Eigen::Vector3d e2 = e3.cross(e1);
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if (e2.norm() < 1e-15) {
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e2 = (std::abs(e1.x()) < 0.9)
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? Eigen::Vector3d::UnitX().cross(e1)
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: Eigen::Vector3d::UnitY().cross(e1);
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}
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e2.normalize();
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e3 = e1.cross(e2).normalized();
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Eigen::Matrix3d R;
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R.col(0) = e1;
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R.col(1) = e2;
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R.col(2) = e3;
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Eigen::AngleAxisd aa(R);
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Eigen::Vector3d r = aa.angle() * aa.axis();
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rod[0] = r.x();
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rod[1] = r.y();
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rod[2] = r.z();
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}
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// Extract rotation (Rodrigues), lengths (a,b,c) and beta (rad) for monoclinic (unique axis b).
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// Frame choice: e2 aligned with b; e1 from a projected orthogonal to e2; e3 = e1 x e2.
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inline void LatticeToRodriguesLengthsBeta_Mono(const CrystalLattice &latt,
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double rod[3],
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double lengths[3],
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double &beta_rad) {
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const Coord a = latt.Vec0();
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const Coord b = latt.Vec1();
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const Coord c = latt.Vec2();
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Eigen::Vector3d A(a[0], a[1], a[2]);
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Eigen::Vector3d B(b[0], b[1], b[2]);
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Eigen::Vector3d C(c[0], c[1], c[2]);
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const double a_len = A.norm();
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const double b_len = B.norm();
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const double c_len = C.norm();
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lengths[0] = a_len;
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lengths[1] = b_len;
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lengths[2] = c_len;
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// beta = angle between a and c
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double cos_beta = 0.0;
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if (a_len > 0.0 && c_len > 0.0)
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cos_beta = std::max(-1.0, std::min(1.0, A.dot(C) / (a_len * c_len)));
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beta_rad = std::acos(cos_beta);
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Eigen::Vector3d e2, ax;
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// e2 along b (unique axis)
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if (b_len > 0.0)
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e2 = B / b_len;
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else
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e2 = Eigen::Vector3d::UnitY();
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if (a_len > 0.0)
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ax = A / a_len;
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else
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ax = Eigen::Vector3d::UnitX();
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Eigen::Vector3d e1 = ax - (ax.dot(e2)) * e2;
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double n1 = e1.norm();
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if (n1 < 1e-15) {
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// Fallback: use any perpendicular to e2
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e1 = (std::abs(e2.x()) < 0.9
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? Eigen::Vector3d::UnitX().cross(e2)
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: Eigen::Vector3d::UnitY().cross(e2));
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}
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e1.normalize();
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// e3 completes the right-handed frame
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Eigen::Vector3d e3 = e1.cross(e2).normalized();
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Eigen::Matrix3d R;
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R.col(0) = e1;
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R.col(1) = e2;
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R.col(2) = e3;
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Eigen::AngleAxisd aa(R);
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Eigen::Vector3d r = aa.angle() * aa.axis();
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rod[0] = r.x();
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rod[1] = r.y();
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rod[2] = r.z();
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}
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CrystalLattice AngleAxisAndLengthsToLattice(const double rod[3], const double lengths[3], bool hex) {
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const Eigen::Vector3d r(rod[0], rod[1], rod[2]);
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const double angle = r.norm();
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Eigen::Matrix3d R = Eigen::Matrix3d::Identity();
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if (angle > 0.0)
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R = Eigen::AngleAxisd(angle, r / angle).toRotationMatrix();
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const Eigen::DiagonalMatrix<double, 3> D(lengths[0], lengths[1], lengths[2]);
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Eigen::Matrix3d Bhex = Eigen::Matrix3d::Identity();
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if (hex) {
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Bhex(0, 1) = -1 / 2.0;
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Bhex(1, 1) = sqrt(3) / 2;
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}
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auto latt = R * D * Bhex;
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return CrystalLattice(Coord(latt(0, 0), latt(1, 0), latt(2, 0)),
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Coord(latt(0, 1), latt(1, 1), latt(2, 1)),
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Coord(latt(0, 2), latt(1, 2), latt(2, 2)));
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}
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inline CrystalLattice AngleAxisLengthsBetaToLattice_Mono(const double rod[3],
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const double lengths[3],
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double beta_rad) {
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const Eigen::Vector3d r(rod[0], rod[1], rod[2]);
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const double angle = r.norm();
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Eigen::Matrix3d R = Eigen::Matrix3d::Identity();
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if (angle > 0.0)
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R = Eigen::AngleAxisd(angle, r / angle).toRotationMatrix();
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const Eigen::DiagonalMatrix<double, 3> D(lengths[0], lengths[1], lengths[2]);
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Eigen::Matrix3d B = Eigen::Matrix3d::Identity();
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// Bmono = [[1,0,cosβ],[0,1,0],[0,0,sinβ]]
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B(0, 2) = std::cos(beta_rad);
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B(2, 2) = std::sin(beta_rad);
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Eigen::Matrix3d latt = R * D * B;
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return CrystalLattice(Coord(latt(0, 0), latt(1, 0), latt(2, 0)),
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Coord(latt(0, 1), latt(1, 1), latt(2, 1)),
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Coord(latt(0, 2), latt(1, 2), latt(2, 2)));
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}
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bool XtalOptimizerInternal(XtalOptimizerData &data,
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const std::vector<SpotToSave> &spots,
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const float tolerance) {
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try {
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data.latt.Regularize(data.crystal_system);
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Coord vec0 = data.latt.Vec0();
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Coord vec1 = data.latt.Vec1();
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Coord vec2 = data.latt.Vec2();
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double beta = data.latt.GetUnitCell().beta;
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// Initial guess for the parameters
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double beam_x = data.geom.GetBeamX_pxl();
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double beam_y = data.geom.GetBeamY_pxl();
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double distance_mm = data.geom.GetDetectorDistance_mm();
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double detector_rot[2] = {data.geom.GetPoniRot1_rad(), data.geom.GetPoniRot2_rad()};
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ceres::Problem problem;
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double latt_vec0[3], latt_vec1[3], latt_vec2[3];
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double rot_vec[3] = {1, 0, 0};
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switch (data.crystal_system) {
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case gemmi::CrystalSystem::Orthorhombic:
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LatticeToRodriguesAndLengths_GS(data.latt, latt_vec0, latt_vec1);
|
||
break;
|
||
case gemmi::CrystalSystem::Tetragonal:
|
||
LatticeToRodriguesAndLengths_GS(data.latt, latt_vec0, latt_vec1);
|
||
latt_vec1[0] = (latt_vec1[0] + latt_vec1[1]) / 2.0;
|
||
break;
|
||
case gemmi::CrystalSystem::Cubic:
|
||
LatticeToRodriguesAndLengths_GS(data.latt, latt_vec0, latt_vec1);
|
||
latt_vec1[0] = (latt_vec1[0] + latt_vec1[1] + latt_vec1[2]) / 3.0;
|
||
break;
|
||
case gemmi::CrystalSystem::Hexagonal:
|
||
LatticeToRodriguesAndLengths_Hex(data.latt, latt_vec0, latt_vec1);
|
||
break;
|
||
case gemmi::CrystalSystem::Monoclinic:
|
||
LatticeToRodriguesLengthsBeta_Mono(data.latt, latt_vec0, latt_vec1, beta);
|
||
latt_vec2[0] = beta;
|
||
latt_vec2[1] = 0.0;
|
||
latt_vec2[2] = 0.0;
|
||
break;
|
||
default:
|
||
// Triclinic: initialize a,b,c and α,β,γ from current unit cell
|
||
LatticeToRodriguesAndLengths_GS(data.latt, latt_vec0, latt_vec1);
|
||
auto uc = data.latt.GetUnitCell();
|
||
latt_vec2[0] = uc.alpha * M_PI / 180.0;
|
||
latt_vec2[1] = uc.beta * M_PI / 180.0;
|
||
latt_vec2[2] = uc.gamma * M_PI / 180.0;
|
||
break;
|
||
}
|
||
|
||
if (data.axis) {
|
||
rot_vec[0] = data.axis->GetAxis().x;
|
||
rot_vec[1] = data.axis->GetAxis().y;
|
||
rot_vec[2] = data.axis->GetAxis().z;
|
||
}
|
||
|
||
const float tolerance_sq = tolerance * tolerance;
|
||
|
||
// Add residuals for each point
|
||
for (const auto &pt: spots) {
|
||
if (!data.index_ice_rings && pt.ice_ring)
|
||
continue;
|
||
|
||
float angle_rad = 0.0;
|
||
|
||
Coord recip = pt.ReciprocalCoord(data.geom);
|
||
|
||
if (data.axis) {
|
||
recip = data.axis->GetTransformationAngle(pt.phi) * recip;
|
||
angle_rad = pt.phi * M_PI / 180.0;
|
||
}
|
||
|
||
double h_fp = recip * vec0;
|
||
double k_fp = recip * vec1;
|
||
double l_fp = recip * vec2;
|
||
|
||
double h = std::round(h_fp);
|
||
double k = std::round(k_fp);
|
||
double l = std::round(l_fp);
|
||
|
||
double norm_sq = (h - h_fp) * (h - h_fp) + (k - k_fp) * (k - k_fp) + (l - l_fp) * (l - l_fp);
|
||
|
||
if (norm_sq > tolerance_sq)
|
||
continue;
|
||
|
||
problem.AddResidualBlock(
|
||
new ceres::AutoDiffCostFunction<XtalResidual, 3, 1, 1, 1, 2, 3, 3, 3, 3>(
|
||
new XtalResidual(pt.x, pt.y,
|
||
data.geom.GetWavelength_A(),
|
||
data.geom.GetPixelSize_mm(),
|
||
angle_rad,
|
||
h, k, l,
|
||
data.crystal_system)),
|
||
nullptr,
|
||
&beam_x,
|
||
&beam_y,
|
||
&distance_mm,
|
||
detector_rot,
|
||
rot_vec,
|
||
latt_vec0,
|
||
latt_vec1,
|
||
latt_vec2
|
||
);
|
||
}
|
||
|
||
if (problem.NumResidualBlocks() < data.min_spots)
|
||
return false;
|
||
|
||
if (!data.refine_distance_mm)
|
||
problem.SetParameterBlockConstant(&distance_mm);
|
||
else {
|
||
const double dist_range = 0.1;
|
||
problem.SetParameterLowerBound(&distance_mm, 0, distance_mm * (1.0 - dist_range));
|
||
problem.SetParameterLowerBound(&distance_mm, 0, distance_mm * (1.0 + dist_range));
|
||
}
|
||
|
||
if (!data.refine_beam_center) {
|
||
problem.SetParameterBlockConstant(&beam_x);
|
||
problem.SetParameterBlockConstant(&beam_y);
|
||
}
|
||
|
||
if (!data.refine_detector_angles) {
|
||
problem.SetParameterBlockConstant(detector_rot);
|
||
} else {
|
||
const double rot_range = 3.0 / 180.0 * M_PI;
|
||
for (int i = 0; i < 2; ++i) {
|
||
problem.SetParameterLowerBound(detector_rot, i, detector_rot[i] - rot_range);
|
||
problem.SetParameterUpperBound(detector_rot, i, detector_rot[i] + rot_range);
|
||
}
|
||
}
|
||
|
||
if (!data.refine_rotation_axis) {
|
||
problem.SetParameterBlockConstant(rot_vec);
|
||
}
|
||
|
||
if (!data.refine_unit_cell) {
|
||
problem.SetParameterBlockConstant(latt_vec1);
|
||
problem.SetParameterBlockConstant(latt_vec2);
|
||
} else {
|
||
// Parameter bounds
|
||
// Lengths
|
||
for (int i = 0; i < 3; ++i) {
|
||
problem.SetParameterLowerBound(latt_vec1, i, data.min_length_A);
|
||
problem.SetParameterUpperBound(latt_vec1, i, data.max_length_A);
|
||
}
|
||
|
||
if (data.crystal_system == gemmi::CrystalSystem::Monoclinic) {
|
||
const double beta_lo = std::max(1e-6, M_PI * (data.min_angle_deg / 180.0));
|
||
const double beta_hi = std::min(M_PI - 1e-6, M_PI * (data.max_angle_deg / 180.0));
|
||
problem.SetParameterLowerBound(latt_vec2, 0, beta_lo);
|
||
problem.SetParameterUpperBound(latt_vec2, 0, beta_hi);
|
||
} else if (data.crystal_system == gemmi::CrystalSystem::Triclinic) {
|
||
// α, β, γ bounds (radians)
|
||
const double alo = M_PI * (data.min_angle_deg / 180.0);
|
||
const double ahi = M_PI * (data.max_angle_deg / 180.0);
|
||
for (int i = 0; i < 3; ++i) {
|
||
problem.SetParameterLowerBound(latt_vec2, i, alo);
|
||
problem.SetParameterUpperBound(latt_vec2, i, ahi);
|
||
}
|
||
}
|
||
}
|
||
|
||
// Configure solver
|
||
ceres::Solver::Options options;
|
||
options.linear_solver_type = ceres::DENSE_QR;
|
||
options.minimizer_progress_to_stdout = false;
|
||
options.max_solver_time_in_seconds = data.max_time;
|
||
options.logging_type = ceres::LoggingType::SILENT;
|
||
options.num_threads = 1; // Fix threads to 1, as this runs in multi-threaded context
|
||
ceres::Solver::Summary summary;
|
||
|
||
// Run optimization
|
||
ceres::Solve(options, &problem, &summary);
|
||
|
||
if (data.refine_beam_center) {
|
||
data.beam_corr_x = data.geom.GetBeamX_pxl() - beam_x;
|
||
data.beam_corr_y = data.geom.GetBeamY_pxl() - beam_y;
|
||
data.geom.BeamX_pxl(beam_x).BeamY_pxl(beam_y);
|
||
}
|
||
|
||
if (data.refine_distance_mm)
|
||
data.geom.DetectorDistance_mm(distance_mm);
|
||
|
||
if (data.refine_detector_angles)
|
||
data.geom.PoniRot1_rad(detector_rot[0]).PoniRot2_rad(detector_rot[1]);
|
||
|
||
if (data.axis && data.refine_rotation_axis)
|
||
data.axis.value().Axis(Coord(rot_vec[0], rot_vec[1], rot_vec[2]));
|
||
|
||
if (data.crystal_system == gemmi::CrystalSystem::Orthorhombic)
|
||
data.latt = AngleAxisAndLengthsToLattice(latt_vec0, latt_vec1, false);
|
||
else if (data.crystal_system == gemmi::CrystalSystem::Tetragonal) {
|
||
latt_vec1[1] = latt_vec1[0];
|
||
data.latt = AngleAxisAndLengthsToLattice(latt_vec0, latt_vec1, false);
|
||
} else if (data.crystal_system == gemmi::CrystalSystem::Cubic) {
|
||
latt_vec1[1] = latt_vec1[0];
|
||
latt_vec1[2] = latt_vec1[0];
|
||
data.latt = AngleAxisAndLengthsToLattice(latt_vec0, latt_vec1, false);
|
||
} else if (data.crystal_system == gemmi::CrystalSystem::Hexagonal) {
|
||
latt_vec1[1] = latt_vec1[0];
|
||
data.latt = AngleAxisAndLengthsToLattice(latt_vec0, latt_vec1, true);
|
||
} else if (data.crystal_system == gemmi::CrystalSystem::Monoclinic) {
|
||
data.latt = AngleAxisLengthsBetaToLattice_Mono(latt_vec0, latt_vec1, latt_vec2[0]);
|
||
} else {
|
||
// Triclinic: reconstruct with generic B from α,β,γ
|
||
const Eigen::Vector3d r(latt_vec0[0], latt_vec0[1], latt_vec0[2]);
|
||
const double angle = r.norm();
|
||
Eigen::Matrix3d R = Eigen::Matrix3d::Identity();
|
||
if (angle > 0.0)
|
||
R = Eigen::AngleAxisd(angle, r / angle).toRotationMatrix();
|
||
|
||
Eigen::Matrix3d B = Eigen::Matrix3d::Identity();
|
||
const double ca = std::cos(latt_vec2[0]);
|
||
const double cb = std::cos(latt_vec2[1]);
|
||
const double cg = std::cos(latt_vec2[2]);
|
||
const double sg = std::sin(latt_vec2[2]);
|
||
|
||
// a along x, b in x-y, c general
|
||
B(0, 0) = 1.0;
|
||
B(1, 0) = 0.0;
|
||
B(2, 0) = 0.0;
|
||
B(0, 1) = cg;
|
||
B(1, 1) = sg;
|
||
B(2, 1) = 0.0;
|
||
|
||
const double cx = cb;
|
||
const double cy = (ca - cb * cg) / sg;
|
||
const double cz = std::sqrt(std::max(0.0, 1.0 - cx * cx - cy * cy));
|
||
|
||
B(0, 2) = cx;
|
||
B(1, 2) = cy;
|
||
B(2, 2) = cz;
|
||
|
||
Eigen::DiagonalMatrix<double, 3> D(latt_vec1[0], latt_vec1[1], latt_vec1[2]);
|
||
Eigen::Matrix3d latt = R * D * B;
|
||
|
||
data.latt = CrystalLattice(Coord(latt(0, 0), latt(1, 0), latt(2, 0)),
|
||
Coord(latt(0, 1), latt(1, 1), latt(2, 1)),
|
||
Coord(latt(0, 2), latt(1, 2), latt(2, 2)));
|
||
}
|
||
data.latt.Regularize(data.crystal_system);
|
||
|
||
return true;
|
||
} catch (...) {
|
||
// Convergence problems, likely not updated
|
||
return false;
|
||
}
|
||
}
|
||
|
||
bool XtalOptimizer(XtalOptimizerData &data, const std::vector<SpotToSave> &spots) {
|
||
if (!XtalOptimizerInternal(data, spots, 0.3))
|
||
return false;
|
||
XtalOptimizerInternal(data, spots, 0.2);
|
||
return XtalOptimizerInternal(data, spots, 0.1);
|
||
}
|