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Jungfraujoch/image_analysis/bragg_integration/BraggIntegrationEngine.cpp
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leonarski_fandClaude Opus 5 5b8ce26c83 integration: the flight path between the sample and the detector is corrected for, and named
A reflection arriving at an angle to the detector normal crosses D/cos(alpha) of
whatever lies between the sample and the sensor, not D, so it is attenuated more than
one arriving head-on and reads low. That is the same geometry as the sensor crossing
already corrected here and the opposite sign, and it was missing.

The factor is exp(D/L*(1/cos(alpha)-1)) from the NIST attenuation coefficient of the
medium, the stated distance and the stated wavelength. Nothing in it is fitted, and
it is not justified by any measured amplitude: the flight path and the sensor
crossing are collinear to better than 0.998 over the angular range any single
experiment samples, so no fit of one can be evidence for the other. It is the
tabulated absorption of a known thickness of a known material over a known path.

The medium cannot be detected. No field of the NXmx application definition describes
it, none of the masters this program reads carries one, and it cannot be inferred
from the implied transmission either - in this corpus a station confirmed to use
helium sits at 51% implied air transmission and one confirmed to use air at 63%, so
any rule separating them is a threshold fitted between two points. It is therefore
assumed, stated, and overridable: --flight-path air|helium|vacuum, defaulting to air.
Helium is its own material rather than an alias for vacuum, attenuating about a six
hundredth of air rather than nothing.

On an untilted detector the correction is a function of resolution alone, so its
entire effect on merged data is a shift in the Wilson B - which is what the report
now prints beside the assumption, accurate to better than a tenth of an angstrom
squared against measurement from 0.05 up to 28. Where that shift is large the report
warns, because a wrong medium is then the largest number in the run: applied to data
from the confirmed helium station it returns a B of 14 A^2 at 3.0 A resolution, which
is not a value a crystal can have.

The corpus contains its own control. One crystal, one station, three collections a
quarter of an hour apart at falling energy through the same air: corrected, the
Wilson B rises monotonically with the dose, as it must.

Co-Authored-By: Claude Opus 5 <noreply@anthropic.com>
Claude-Session: https://claude.ai/code/session_01EFEJG6WBQv8th4UJFNe53N
2026-09-05 17:55:43 +02:00

242 lines
12 KiB
C++

// SPDX-FileCopyrightText: 2026 Filip Leonarski, Paul Scherrer Institute <filip.leonarski@psi.ch>
// SPDX-License-Identifier: GPL-3.0-only
#include "BraggIntegrationEngine.h"
#include <algorithm>
#include <cmath>
#include <map>
#include <mutex>
#include <numeric>
#include <string>
#include <tuple>
#include "../../common/JFJochMath.h" // PI (M_PI is not standard, and MSVC does not define it)
#include "../SensorAbsorption.h"
namespace {
// Radial parallax broadening as the coefficient of tan^2(2theta), i.e. Var(z)/pixel^2 [px^2].
// Copied verbatim from ProfileIntegrate2D: a photon converts at a random depth z (exponential,
// attenuation length L, truncated at the sensor thickness), shifting the recorded spot radially by
// z*tan(2theta). L comes from the tabulated NIST attenuation coefficients (SensorAbsorption.h); the
// lambda^3 approximation this used before is within 0.2% for silicon above 10 keV but overstates
// the attenuation length of CdTe by up to a factor of two, and by six above the Cd K edge, which
// made this variance 1.9x too large on 750 um CdTe data.
double parallax_var_px2(const std::string &material, double thickness_um, double lambda_A, double pixel_um) {
if (!(thickness_um > 0.0) || !(pixel_um > 0.0) || !(lambda_A > 0.0))
return 0.0;
const double L = sensor_absorption::AttenuationLength_um(material, lambda_A);
if (!(L > 0.0))
return 0.0;
const double a = thickness_um / L, e = std::exp(-a);
if (1.0 - e <= 0.0)
return 0.0;
const double mean = L * (1.0 - (1.0 + a) * e) / (1.0 - e);
const double ez2 = L * L * (2.0 - (a * a + 2.0 * a + 2.0) * e) / (1.0 - e);
const double var = std::max(0.0, ez2 - mean * mean); // um^2
return var / (pixel_um * pixel_um);
}
// The radial-offset kernels below are a pure function of these six numbers, and one engine is built
// per worker per pass - 96 of them on a two-pass run - so the table was built 96 times over from the
// same inputs. Build it once and let the rest copy it; it is a few hundred floats. Two workers can
// still race to build the same table, which costs nothing but the second build: the values are
// identical, and emplace keeps whichever arrived first.
struct RadialKernelKey {
float r1_sq, r2, r3;
int n_kern, k_off, k_len;
bool operator<(const RadialKernelKey &o) const {
return std::tie(r1_sq, r2, r3, n_kern, k_off, k_len)
< std::tie(o.r1_sq, o.r2, o.r3, o.n_kern, o.k_off, o.k_len);
}
};
std::mutex radial_kernel_mutex;
std::map<RadialKernelKey, std::vector<float>> radial_kernel_cache;
} // namespace
BraggIntegrationEngine::BraggIntegrationEngine(const DiffractionExperiment &experiment)
: geom(experiment.GetDiffractionGeometry()) {
const auto settings = experiment.GetBraggIntegrationSettings();
const auto &det = experiment.GetDetectorSetup();
mode = settings.GetIntegrator();
empirical = mode == IntegratorMode::ProfileEmpirical;
// Same frame as the reflections' predicted_x/predicted_y and the ImagePreprocessorBuffer that
// feeds this engine (MXAnalysisWithoutFPGA sizes that buffer to GetPixelsNum()).
xpixel = experiment.GetXPixelsNum();
ypixel = experiment.GetYPixelsNum();
npixel = experiment.GetPixelsNum();
r1_sq = settings.GetR1() * settings.GetR1();
r2 = settings.GetR2();
r2_sq = r2 * r2;
r3 = settings.GetR3();
r3_sq = r3 * r3;
R = static_cast<int>(std::ceil(r2));
G = 2 * R + 1;
GG = G * G;
// The X-ray bandwidth enters ONE place: it smears a reflection radially by bw_sigma * Rpx, which
// the per-reflection Gaussian carries as part of its radial variance. It is not a mode switch -
// the background estimator and the parallax/capture term below are the same whatever the beam is.
bw_sigma = experiment.GetBandwidthFWHM().value_or(0.0f) / 2.3548f;
const double c_par = parallax_var_px2(det.GetSensorMaterial(), det.GetSensorThickness_um(),
geom.GetWavelength_A(), geom.GetPixelSize_mm() * 1000.0);
c_radial = c_par + bragg_engine::C_CAPTURE;
F_px = geom.GetDetectorDistance_mm() / std::max(1e-6f, geom.GetPixelSize_mm());
beam_x = geom.GetBeamX_pxl();
beam_y = geom.GetBeamY_pxl();
use_ellipse = !empirical;
// Per-reflection signal/background geometry: the ring elongated radially by k_sigma times the
// beam's own radial streak, capped. k_sigma = 0 is the fixed circular stencil, bit for bit, and
// so is any monochromatic beam, where the streak is zero.
stencil.beam_x = beam_x;
stencil.beam_y = beam_y;
stencil.r2 = r2;
stencil.r3 = r3;
stencil.bw_sigma = static_cast<float>(bw_sigma);
stencil.k_sigma = settings.GetStencilKSigma();
stencil.max_grow = bragg_engine::MAX_STENCIL_GROW_OVER_R3 * r3;
// Robust background ring, one estimator or the other (see BraggIntegrationSettings): a high-side
// sigma-clip (rugnux --background-clip, the default) or, when the clip is switched off, a
// symmetric trimmed mean (rugnux --background-trim). The caller owns the choice - the engine no
// longer overrides it for broadband data.
bkg_clip_nsigma = settings.GetBackgroundClipNSigma();
bkg_trim = bkg_clip_nsigma > 0.0f ? 0.0f : settings.GetBackgroundTrimFraction();
// Overlap treatment. Ownership is decided out to the fit grid's half size, which is where the
// profile fit reads pixels; beyond it a pixel that nobody claims is this reflection's own.
// Excluding the shared pixels needs a profile to renormalise, so it cannot act on a box sum -
// drop it to Off there rather than build an owner map nothing will read.
overlap = settings.GetOverlap();
if (overlap == OverlapMode::Exclude && mode == IntegratorMode::BoxSum)
overlap = OverlapMode::Off;
overlap_min_peak = settings.GetOverlapMinPeak();
claim = static_cast<float>(R);
inv_claim = 1.0f / claim;
// Radial-offset kernels for the background curvature correction. A stencil pixel at (dx, dy)
// sits at radial offset dx*cos(phi) + dy*sin(phi) from the reflection, where phi is the
// reflection's azimuth; averaging over phi makes the kernels position-independent, which is
// exact to the extent the stencil is small against the reflection's radius (r3 = 10 px vs
// hundreds). k_diff is the annulus histogram minus the disk histogram, each normalised, so
// dot(k_diff, B) is directly mean_annulus(B) - mean_disk(B).
// Unset = auto: start off, and let the analysis raise it per image where the ice score says the
// background really is radial. An engine nobody drives therefore never applies the correction.
const auto radial = settings.GetBackgroundRadialCorrection();
bkg_radial_auto = !radial.has_value();
bkg_radial = radial.value_or(false);
// The table spans zero growth up to whatever the widest reflection on this detector reaches, one
// kernel per pixel of growth; with nothing elongated a single kernel is all there is, which is
// the layout and the values of every build before the stencil existed. It is built only when the
// correction can ever run - the rows are not cheap, and nothing may read them otherwise:
// bkg_radial is raised after construction only by the auto mode (MXAnalysisWithoutFPGA), which
// requires bkg_radial_auto, and the GPU allocates its curve buffers under the same condition.
// n_kern is the largest row BraggStencilKernelIndex can select, plus one.
r_max = std::hypot(std::max<double>(beam_x, static_cast<double>(xpixel) - beam_x),
std::max<double>(beam_y, static_cast<double>(ypixel) - beam_y));
bkg_radial_built = bkg_radial || bkg_radial_auto;
const float grow_max = bkg_radial_built ? BraggStencilGrow_px(static_cast<float>(r_max), stencil)
: 0.0f;
n_kern = static_cast<int>(std::lround(grow_max)) + 1;
// Every row must fit: the last one is built at grow = n_kern - 1, which rounding can put just
// above grow_max.
k_off = static_cast<int>(std::ceil(r3 + std::max<double>(grow_max, n_kern - 1))) + 1;
k_len = 2 * k_off + 1;
const RadialKernelKey kernel_key{r1_sq, r2, r3, n_kern, k_off, k_len};
{
const std::lock_guard lock(radial_kernel_mutex);
if (const auto it = radial_kernel_cache.find(kernel_key); it != radial_kernel_cache.end())
k_diff = it->second;
}
if (k_diff.empty()) {
k_diff.reserve(static_cast<size_t>(n_kern) * k_len);
for (int j = 0; j < n_kern; ++j)
BuildRadialKernel(static_cast<float>(j));
const std::lock_guard lock(radial_kernel_mutex);
radial_kernel_cache.emplace(kernel_key, k_diff);
}
polarization = experiment.GetPolarizationFactor();
}
void BraggIntegrationEngine::BuildRadialKernel(float grow) {
// Histogram the stencil over radial offset, averaged over azimuth so the kernel does not depend
// on where the reflection sits. The average is over the SUB-PIXEL PHASE of the detector grid
// against the radial direction, not over the stencil's own orientation: the stencil is built in
// the reflection's frame at each azimuth, so an elongated one stays aligned with the radius, as
// it is on the detector. k_diff is the annulus histogram minus the disk histogram, each
// normalised, so dot(k_diff, B) is directly mean_annulus(B) - mean_disk(B).
// The signal disk is a circle whatever the ring does, so its histogram is the same for every
// kernel in the table - build it once.
const bool first = hist_disk.empty();
if (first)
hist_disk.assign(k_len, 0.0);
std::vector<double> hist_ann(k_len, 0.0);
constexpr int n_phi = 512;
const int span = static_cast<int>(std::ceil(r3 + grow)) + 1;
const float si = r2 / (r2 + grow), so = r3 / (r3 + grow);
const double q_in = 1.0 - static_cast<double>(si) * si;
const double q_out = 1.0 - static_cast<double>(so) * so;
for (int p = 0; p < n_phi; ++p) {
const double phi = 2.0 * PI * p / n_phi, cp = std::cos(phi), sp = std::sin(phi);
for (int dy = -span; dy <= span; ++dy)
for (int dx = -span; dx <= span; ++dx) {
const double d2 = static_cast<double>(dx) * dx + static_cast<double>(dy) * dy;
const double rad = dx * cp + dy * sp;
const int k = k_off + static_cast<int>(std::lround(rad));
if (k < 0 || k >= k_len)
continue;
const double rad2 = rad * rad;
if (d2 < r1_sq) {
if (first) hist_disk[k] += 1.0;
} else if (d2 - q_in * rad2 >= r2_sq && d2 - q_out * rad2 < r3_sq) {
hist_ann[k] += 1.0;
}
}
}
if (first) sum_disk = std::accumulate(hist_disk.begin(), hist_disk.end(), 0.0);
const double sd = sum_disk;
const double sa = std::accumulate(hist_ann.begin(), hist_ann.end(), 0.0);
for (int k = 0; k < k_len; ++k)
k_diff.push_back(static_cast<float>(hist_ann[k] / sa - hist_disk[k] / sd));
}
std::vector<Reflection> BraggIntegrationEngine::Finalize(const std::vector<Reflection> &predicted,
size_t npredicted,
const std::vector<BraggFitResult> &results,
int64_t image_number) const {
std::vector<Reflection> out;
out.reserve(npredicted);
for (size_t i = 0; i < npredicted; ++i) {
const auto &fr = results[i];
if (!fr.ok)
continue;
Reflection refl = predicted[i];
refl.I = fr.I;
refl.sigma = fr.sigma;
refl.bkg = fr.bkg;
refl.var_bkg = fr.var_bkg;
if (fr.has_observed) {
refl.observed_x = fr.observed_x;
refl.observed_y = fr.observed_y;
}
refl.observed = true;
if (polarization)
refl.prescaling_corr /= geom.CalcAzIntPolarizationCorr(refl.predicted_x, refl.predicted_y, polarization.value());
refl.image_scale_corr = refl.prescaling_corr * refl.qe_corr * refl.flight_corr / refl.partiality;
refl.image_number = static_cast<float>(image_number);
out.push_back(refl);
}
return out;
}