Three terms of the score of a model - the same F_model at every stage, the as-given start and the refined end alike - and a breakdown of it: - Riding hydrogens from the start: the dictionary's hydrogens are added before the model is first scored (REFMAC's 0-cycle restores them; they move R by 0.010-0.013 at 1.1 A). The engine is made once, with them. - The bulk-solvent mask on a grid of its own, min(d_min/3, 0.4 A), at most 2^26 points. On the density grid (1.1 A at 3.3 A) gemmi's 0.8 A shrink found no grid offset and was skipped, which put R 0.015-0.03 high at >= 2.5 A. 0.3 and 0.4 A agree to 0.001. - The overall scale and anisotropic B by robust least squares (pseudo-Huber, iteratively reweighted, c = median |residual|) in the fine pass of the k_sol/b_sol grid (ModelScaleBox::robust, refinement only; MR and validation keep the plain fit). Plain least squares on |F| is the exact LS optimum but lets a few badly-fitted strong reflections set the scale (1.1 A set: R 0.1706 against REFMAC's 0.1600). The scale fit of refinement now runs on the CPU (no ModelScaleGPUPool). RefinementSettings::score_only scores the model as given and stops; RefinementResult::score_start carries every term (k, B, anisotropic B, k_sol, b_sol, mask spacing, R in 20 shells, -lnL work/free, the likelihood FOM, hydrogens; per-reflection terms with score_only). GeometryStatistics gains rmsZ. rugnux_refine_test: --score-only, --dump. Measured against REFMAC 5.8.0431 ncyc 0 (refi bref iso) on the same model, data and flags, 14 open-arm sets 1.1-3.6 A: R-work/R-free within 0.002 on 12 (was +0.003..+0.03); 7n2s and 9yl4 score 0.003/0.005 below REFMAC, which a 0.6-0.8 A mask grid reproduces. REFMAC with ANISOU stripped scores identically, so isotropic B is not a parity term. Open: the likelihood's D/FOM (ours 0.01-0.11 higher at high resolution); geometry differs only by REFMAC's metal LINK restraints and residues outside the embedded dictionary. Co-Authored-By: Claude Opus 5.5 <noreply@anthropic.com> Claude-Session: https://claude.ai/code/session_015CeEGgpKdfkCTJb3YNMJcu (cherry picked from commit 4f94b21611874ad9dcf89e6771fe311a0e10bb06) (cherry picked from commit 00db6a6f539ac2da515c0a649474335f4c4b07b8)
175 lines
9.2 KiB
C++
175 lines
9.2 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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#pragma once
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#include <array>
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#include <chrono>
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#include <cstdint>
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#include <complex>
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#include <memory>
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#include <optional>
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#include <vector>
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#include "gemmi/grid.hpp"
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#include "gemmi/model.hpp"
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#include "gemmi/symmetry.hpp"
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#include "gemmi/unitcell.hpp"
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#include "../../common/Reflection.h" // MergedReflection
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#include "RefinementRestraints.h" // RestraintSet
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#include "RigidBodyRefine.h" // SymmetryComposition
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class Logger;
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// The X-ray side of restrained refinement (Refinement.h): the observed amplitudes, the model's structure
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// factors and the maximum-likelihood target that compares them, with its gradient with respect to every
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// atom's position and B.
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// The reflections a refinement fits and scores: the observed amplitudes, in the group's reciprocal ASU, that
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// the refinement grid composes (SymmetryComposition) - every observed one in practice.
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struct RefinementReflections {
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std::vector<gemmi::Miller> hkl;
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std::vector<float> fo, sigma;
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std::vector<char> free, centric;
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std::vector<float> epsilon;
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std::vector<double> inv_d2;
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size_t Size() const { return hkl.size(); }
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};
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// The French-Wilson amplitudes of `merged` (NaN dropped) into the ASU of `sg`, those the grid of
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// RigidBodyZoneGrid(cell, sg, d_min) composes.
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RefinementReflections PrepareRefinementReflections(const std::vector<MergedReflection> &merged,
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const gemmi::UnitCell &cell, const gemmi::SpaceGroup &sg,
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double d_min);
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// What turns the atoms' structure factors F into the model the target compares with the data, per reflection:
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// F_model = k_total (F + fmask),
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// with k_total the overall scale and anisotropic B and fmask the bulk solvent already scaled by k_sol
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// exp(-b_sol s^2/4); and the two parameters of the likelihood, D and the variance. Fixed for one macro-cycle.
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struct XrayRowModel {
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std::vector<float> k_total;
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std::vector<std::complex<float>> fmask;
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std::vector<float> d, var;
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};
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// The flat bulk-solvent model's mask (SolventMasker with the Refmac radii, PutMaskOnGrid) and its structure factors
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// at the reflections, on a grid of its own rather than the atoms' density grid: the mask's edge is set by the
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// probe and shrink radii (1.0 and 0.8 A), which a grid at d_min / 3 cannot resolve at low resolution - at 3 A
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// its 1 A step leaves no grid point within the shrink radius and the shrink is skipped. The step is therefore
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// d_min / 3 or MASK_SPACING_MAX, whichever is finer - where the mask grid stays within MASK_POINTS_MAX points; a
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// cell too large for that gets the spacing that fills it. The R-factors of low-resolution models settle at a
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// step of 0.4 A (within 0.001 of 0.3 A) and move by up to 0.005 between 0.4 and 0.8 A.
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// The flat solvent model of Fokine & Urzhumtsev (2002) Acta Cryst. D58, 1387-1392
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class BulkSolventMask {
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public:
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static constexpr double MASK_SPACING_MAX = 0.4; // A
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static constexpr double MASK_POINTS_MAX = 1 << 26;
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BulkSolventMask(const gemmi::UnitCell &cell, const gemmi::SpaceGroup &sg, double d_min, size_t nthreads);
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// Fmask (unscaled) of `model` at `hkl`.
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void Fmask(const gemmi::Model &model, const std::vector<gemmi::Miller> &hkl,
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std::vector<std::complex<float>> &f) const;
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double Spacing() const { return spacing_; }
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private:
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gemmi::Grid<float> grid_;
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std::vector<size_t> orbit_leaders_;
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size_t nthreads_;
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double spacing_;
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};
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// The ML parameters per reflection from the free reflections: D and beta fitted by maximum likelihood in
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// resolution bins of the free set and interpolated between the bins' centres; the variance of a reflection is
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// epsilon beta + sigma^2. `fmodel` is k_total (F + fmask), without D.
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// Following Lunin & Skovoroda (1995) Acta Cryst. A51, 880-887, and Afonine et al. (2012) Acta Cryst. D68, 352-367
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void EstimateLikelihoodParameters(const RefinementReflections &refl, const std::vector<std::complex<float>> &fmodel,
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XrayRowModel &rows, size_t nthreads = 1);
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// R-work and R-free of k_total (F + fmask) against the observations.
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struct RFactors {
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double r_work = 1, r_free = 1;
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int n_work = 0, n_free = 0;
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};
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RFactors ComputeRFactors(const RefinementReflections &refl, const std::vector<std::complex<float>> &fmodel);
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// x, y, z and B of every atom of `model`, in model order.
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std::vector<std::array<double, 4>> ModelXyzB(const gemmi::Model &model);
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// What evaluates the targets for a set of atom positions and B: the CPU below, or a GPU (RefinementGPU.h). The
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// atoms are the model's, all of them, in model order; the grid and the reflections are fixed when the engine is
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// made, the row model each macro-cycle, the blur where SetBlur is called.
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class RefinementEngine {
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public:
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virtual ~RefinementEngine() = default;
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// The blur the atoms are gridded with (DensityCalculator's), and the matching unblur of their transform.
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// Every atom's B must stay above what the blur was chosen for (RefinementBlur) while it is in use.
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virtual void SetBlur(double blur) = 0;
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virtual void SetRowModel(const XrayRowModel &rows) = 0;
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// F of the atoms at the reflections.
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virtual void Fcalc(const gemmi::Model &model, std::vector<std::complex<float>> &f) = 0;
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// The bulk-solvent mask's structure factors at the reflections (unscaled).
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virtual void Fmask(const gemmi::Model &model, std::vector<std::complex<float>> &f) = 0;
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// The sum of -ln L over the working reflections and, with `grad`, its derivatives with respect to every
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// atom's x, y, z (Cartesian, A) and B (A^2), in model order.
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virtual double Evaluate(const gemmi::Model &model, std::vector<std::array<double, 4>> *grad) = 0;
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virtual bool OnGPU() const = 0;
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// Restraint set `which` (0: the geometry and the repulsions, 1: the B similarity) and its sum of E at xyzb
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// (x, y, z, B per atom) with, given `grad`, dE/d(x, y, z, B) per atom. On the CPU unless the engine has its own.
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virtual void SetRestraints(int which, const RestraintSet &set) { restraints_[which] = set; }
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virtual double EvaluateRestraints(int which, const std::vector<std::array<double, 4>> &xyzb,
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std::vector<std::array<double, 4>> *grad) {
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if (grad != nullptr)
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grad->assign(xyzb.size(), {0, 0, 0, 0});
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return ::EvaluateRestraints(restraints_[which], xyzb, grad);
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}
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// Evaluate() and EvaluateRestraints(which) at the atoms of `model` as they are, in one go: returns the X-ray
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// target, and the restraints' sum in `restraints`.
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virtual double EvaluateWithRestraints(const gemmi::Model &model, int which, std::vector<std::array<double, 4>> *grad,
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std::vector<std::array<double, 4>> *restraint_grad, double &restraints) {
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const double xray = Evaluate(model, grad);
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restraints = EvaluateRestraints(which, ModelXyzB(model), restraint_grad);
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return xray;
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}
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private:
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RestraintSet restraints_[2];
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};
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// The time a refinement spends in one stage, summed over every call (and over threads) until Log(): the scope of
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// an instance is one call, and an NVTX range of the stage's name.
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class RefinementStage {
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public:
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explicit RefinementStage(const char *name);
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~RefinementStage();
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RefinementStage(const RefinementStage &) = delete;
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RefinementStage &operator=(const RefinementStage &) = delete;
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// "TIMING refine.<stage> <seconds> <calls>" per stage at debug level, then the sums start again.
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static void Log(Logger &logger);
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private:
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const char *name_;
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std::chrono::steady_clock::time_point start_;
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uint64_t nvtx_;
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};
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// The blur for a model whose smallest B may go as low as b_floor: DensityCalculator's
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// set_refmac_compatible_blur() for that B, on the refinement grid of d_min.
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double RefinementBlur(const gemmi::UnitCell &cell, const gemmi::SpaceGroup &sg, double d_min, double b_floor);
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// The CPU engine: the density of one copy of the atoms on the grid of RigidBodyZoneGrid(cell, sg, d_min)
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// (PutModelDensityOnGrid), its transform and the crystal's symmetry composed in reciprocal space
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// (SymmetryComposition). The gradient by the FFT method: the derivative of the target with respect to each
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// structure factor, taken back to real space by one inverse transform, is a map; each atom's derivatives are
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// that map summed against the derivatives of its own density.
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// Following Agarwal (1978) Acta Cryst. A34, 791-809
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std::unique_ptr<RefinementEngine> MakeRefinementEngineCPU(const gemmi::UnitCell &cell,
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const gemmi::SpaceGroup &sg, double d_min,
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const RefinementReflections &refl, size_t nthreads);
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// The derivative map of the X-ray target on a grid (the FFT method's map), summed against each atom's density
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// derivatives: dT/d(x, y, z, B) per atom. `map` is u fastest on the grid of RigidBodyZoneGrid(), the atoms
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// gridded with `blur`. Exposed for the tests.
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void AtomGradientsFromMap(const gemmi::Grid<float> &map, const gemmi::Model &model, double blur, size_t nthreads,
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std::vector<std::array<double, 4>> &grad);
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