Two independent pieces in the same code path. The background-estimate variance was never propagated. A reflection's background comes from a finite ring of n_b pixels, so subtracting it adds var(B)/n_b per signal pixel - sqrt(1 + n_d/n_b) = 1.109 with the shipped stencil. Both engines omitted it, which is exactly the 1.11-1.19 gap measured between the off-ring scatter and the reported sigma. Three lines each; it affects every dataset, not only iced ones. The radial correction is new and OFF by default (--background-radial). The signal disk and the background ring are concentric, so for any background LINEAR in position <B>_ann == <B>_disk identically and a plane fit buys nothing; the leading error is the CURVATURE of the radial background, which on a sharp ice ring reaches +26 counts on a single reflection. Since every reflection uses the same stencil, that error is a fixed kernel over radial offset - one short dot product per reflection and no extra pixel reads. Validated on empty apertures before any C++: mean |bias| over 9 bands / 3 crystals 4.33 -> 0.79 counts with the scatter unchanged. Three things it cost a battery each to learn, all now in the code: - the radial curve must be accumulated from CLIPPED annulus pixels, inside the clip pass, or it carries neighbour tails and zingers (so it is inert under --integrator boxsum, which has no clip pass); - the GPU version was a 1.8x slowdown from atomicAdd contention on a small radial array - staged in shared memory per block it now costs nothing measurable; - it is battery-NEUTRAL as a default, because the reflections whose bias it fixes are the ones the ice handling already excludes. Hence off by default. CPU/GPU parity extended with two radial sections: 9002 assertions. Also fixes a latent French-Wilson quadrature collapse: j_max = I + 8 sigma on a fixed 400-point grid degenerates to a single cell once sigma >> 50 <I>, giving F = 0.1 sqrt(sigma) with sigmaF -> 0. Harmless today, but any sigma-inflation scheme detonates it. Co-Authored-By: Claude Opus 5 (1M context) <noreply@anthropic.com>
174 lines
7.8 KiB
C++
174 lines
7.8 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 "FrenchWilson.h"
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#include <algorithm>
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#include <cmath>
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#include <future>
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#include <limits>
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#include <vector>
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#include "../../common/ResolutionShells.h"
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#include "gemmi/symmetry.hpp"
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namespace {
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struct Posterior {
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double mean_I; // <J> (posterior mean true intensity)
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double mean_F; // <|F|> (posterior mean amplitude)
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};
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// Posterior moments of the true intensity J >= 0 given a measurement I +/- sigma and the Wilson
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// prior with mean sigma_wilson. Integrated numerically over J in [0, I + 8 sigma] with a log-shift
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// so the exponentials never overflow/underflow. acentric: p(J) ~ exp(-J/S); centric:
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// p(J) ~ exp(-J/2S)/sqrt(J).
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// `logw` is caller-owned scratch of npts doubles (one per worker), so the integration allocates nothing.
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Posterior integrate_posterior(double I, double sigma, double sigma_wilson, bool centric, int npts,
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std::vector<double> &logw) {
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const double inv_2s2 = 1.0 / (2.0 * sigma * sigma);
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// The posterior is the Gaussian likelihood tilted by the exponential prior, so it peaks at
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// I - sigma^2/S and decays over whichever of sigma and S is TIGHTER. Ranging to I + 8 sigma
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// regardless is wrong once sigma greatly exceeds S: with npts fixed the whole prior then falls
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// inside the first grid cell, the quadrature degenerates to that one point and returns
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// F = sqrt(dj/2) with sigmaF -> 0 - i.e. a reflection we know nothing about comes back looking
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// like the best measured one in the file.
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const double prior_scale = centric ? 2.0 * sigma_wilson : sigma_wilson;
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const double peak = std::max(I - sigma * sigma / prior_scale, 0.0);
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const double width = peak > 0.0 ? sigma : std::min(sigma, prior_scale);
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const double j_max = peak + 10.0 * width;
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const double dj = j_max / npts;
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double max_logw = -std::numeric_limits<double>::infinity();
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for (int i = 0; i < npts; ++i) {
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const double j = (i + 0.5) * dj;
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const double diff = I - j;
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const double log_prior = centric ? (-j / (2.0 * sigma_wilson) - 0.5 * std::log(j))
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: (-j / sigma_wilson);
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logw[i] = log_prior - diff * diff * inv_2s2;
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max_logw = std::max(max_logw, logw[i]);
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}
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double sum_w = 0, sum_wI = 0, sum_wF = 0;
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for (int i = 0; i < npts; ++i) {
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const double j = (i + 0.5) * dj;
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const double w = std::exp(logw[i] - max_logw);
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if (!std::isfinite(w))
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continue;
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sum_w += w;
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sum_wI += w * j;
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sum_wF += w * std::sqrt(j);
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}
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if (sum_w <= 0.0) {
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const double j = std::max(I, 0.0);
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return {j, std::sqrt(j)};
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}
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return {sum_wI / sum_w, sum_wF / sum_w};
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}
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} // namespace
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void ApplyFrenchWilson(std::vector<MergedReflection> &merged, int32_t space_group_number,
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const FrenchWilsonOptions &opts) {
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// Naive amplitude sqrt(max(I,0)) for a missing / strong / untrusted intensity; NaN in -> NaN out
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// (a missing Bijvoet hand stays missing). Fills one (F, sigmaF) pair.
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auto naive_one = [](float I, float sigma, float &F, float &sigF) {
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if (!std::isfinite(I)) { F = NAN; sigF = NAN; return; }
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const double ip = std::max(I, 0.0f);
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F = static_cast<float>(std::sqrt(ip));
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sigF = (ip > 0.0 && std::isfinite(sigma)) ? static_cast<float>(sigma / (2.0 * std::sqrt(ip))) : NAN;
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};
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// The mean intensity and each measured hand share the reflection's Wilson prior, so fill all three.
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auto naive_all = [&](MergedReflection &r) {
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naive_one(r.I, r.sigma, r.F, r.sigmaF);
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naive_one(r.I_plus, r.sigma_plus, r.F_plus, r.sigmaF_plus);
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naive_one(r.I_minus, r.sigma_minus, r.F_minus, r.sigmaF_minus);
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};
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const gemmi::SpaceGroup *sg = gemmi::find_spacegroup_by_number(space_group_number);
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if (sg == nullptr || merged.empty()) {
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for (auto &r : merged) naive_all(r);
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return;
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}
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const gemmi::GroupOps gops = sg->operations();
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float d_min = std::numeric_limits<float>::max(), d_max = 0.0f;
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for (const auto &r : merged)
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if (std::isfinite(r.d) && r.d > 0.0f) {
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d_min = std::min(d_min, r.d);
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d_max = std::max(d_max, r.d);
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}
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if (!(d_min < d_max && d_min > 0.0f)) {
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for (auto &r : merged) naive_all(r);
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return;
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}
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// Wilson mean intensity <I/epsilon> per resolution shell.
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ResolutionShells shells(d_min * 0.999f, d_max * 1.001f, opts.num_shells);
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std::vector<double> shell_sum(opts.num_shells, 0.0);
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std::vector<int> shell_count(opts.num_shells, 0);
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double global_sum = 0.0;
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int global_count = 0;
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auto epsilon = [&](const MergedReflection &r) {
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return std::max(1, gops.epsilon_factor_without_centering({{r.h, r.k, r.l}}));
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};
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for (const auto &r : merged) {
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if (!std::isfinite(r.I) || !std::isfinite(r.sigma) || r.sigma <= 0.0f)
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continue;
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const double i_over_eps = r.I / epsilon(r);
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global_sum += i_over_eps;
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++global_count;
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if (const auto s = shells.GetShell(r.d)) {
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shell_sum[*s] += i_over_eps;
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++shell_count[*s];
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}
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}
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const double global_mean = global_count > 0 ? std::max(global_sum / global_count, 1e-10) : 1.0;
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std::vector<double> shell_mean(opts.num_shells, global_mean);
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for (int s = 0; s < opts.num_shells; ++s)
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if (shell_count[s] >= opts.min_reflections_per_shell)
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shell_mean[s] = std::max(shell_sum[s] / shell_count[s], 1e-10);
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// French-Wilson |F| for one intensity of reflection r (its mean, or one Bijvoet hand); the shell
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// Wilson prior, epsilon and centric flag are the reflection's, shared by all three.
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auto fw_one = [&](const MergedReflection &r, float I, float sigma, float &F, float &sigF,
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std::vector<double> &logw) {
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if (!std::isfinite(I) || !std::isfinite(sigma) || sigma <= 0.0f) { naive_one(I, sigma, F, sigF); return; }
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// Strong reflections: the FW correction is negligible, <|F|> = sqrt(I).
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if (I > opts.strong_cutoff * sigma) { naive_one(I, sigma, F, sigF); return; }
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const auto s = shells.GetShell(r.d);
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const double sigma_wilson = epsilon(r) * (s ? shell_mean[*s] : global_mean);
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const bool centric = gops.is_reflection_centric({{r.h, r.k, r.l}});
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const Posterior post = integrate_posterior(I, sigma, sigma_wilson, centric,
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opts.integration_points, logw);
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F = static_cast<float>(post.mean_F);
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sigF = static_cast<float>(std::sqrt(std::max(0.0, post.mean_I - post.mean_F * post.mean_F)));
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};
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// Each reflection's amplitudes depend only on itself and the shell priors above, so the loop is
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// data-parallel over contiguous chunks and gives the same result whatever the worker count.
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const int n = static_cast<int>(merged.size());
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const int nt = std::clamp(opts.num_threads, 1, n);
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const int chunk = (n + nt - 1) / nt;
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auto do_chunk = [&](int lo, int hi) {
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std::vector<double> logw(opts.integration_points);
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for (int i = lo; i < hi; ++i) {
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MergedReflection &r = merged[i];
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fw_one(r, r.I, r.sigma, r.F, r.sigmaF, logw);
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fw_one(r, r.I_plus, r.sigma_plus, r.F_plus, r.sigmaF_plus, logw);
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fw_one(r, r.I_minus, r.sigma_minus, r.F_minus, r.sigmaF_minus, logw);
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}
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};
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if (nt == 1) {
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do_chunk(0, n);
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return;
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}
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std::vector<std::future<void>> futures;
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futures.reserve(nt);
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for (int t = 0; t < nt; ++t) {
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const int lo = t * chunk, hi = std::min(n, lo + chunk);
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if (lo >= hi) break;
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futures.emplace_back(std::async(std::launch::async, [&do_chunk, lo, hi] { do_chunk(lo, hi); }));
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}
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for (auto &f : futures) f.get();
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}
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