Files
Jungfraujoch/tests/WriteReflectionsTest.cpp
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

140 lines
6.5 KiB
C++

// SPDX-FileCopyrightText: 2026 Filip Leonarski, Paul Scherrer Institute <filip.leonarski@psi.ch>
// SPDX-License-Identifier: GPL-3.0-only
#include <catch2/catch_all.hpp>
#include <filesystem>
#include <string>
#include <gemmi/mtz.hpp>
#include "../common/DiffractionExperiment.h"
#include "../image_analysis/WriteReflections.h"
#include "../image_analysis/IntegrationOutcome.h"
#include <cmath>
#include "SyntheticMergedReflections.h"
namespace {
// The wavelength CCP4's mtzlib substitutes when the data columns belong to dataset 0, which it
// takes for the reserved HKL_base: Cu K-alpha, and the wrong edge for anything reading f'/f''
// out of the file.
constexpr double CU_KALPHA_A = 1.54187;
constexpr UnitCell TETRAGONAL_CELL{47.0f, 47.0f, 63.0f, 90.0f, 90.0f, 90.0f};
DiffractionExperiment TestExperiment() {
DiffractionExperiment x;
x.IncidentEnergy_keV(12.7f); // ~0.976 A, nowhere near the Cu K-alpha default
x.SpaceGroupNumber(96); // P 43 21 2
x.SetUnitCell(TETRAGONAL_CELL);
return x;
}
}
TEST_CASE("Merged MTZ: the data dataset is id 1 and carries the wavelength", "[write_reflections]") {
jfjoch_test::SyntheticMergeParams params;
params.true_space_group = "P 43 21 2";
params.twin_supergroup = "P 43 21 2";
params.d_min_A = 5.0;
const auto reflections = jfjoch_test::GenerateSyntheticMerged(params);
REQUIRE(!reflections.empty());
const auto experiment = TestExperiment();
const auto path = (std::filesystem::temp_directory_path() / "rugnux_merged_wavelength.mtz").string();
WriteMtzReflections(reflections, TETRAGONAL_CELL, experiment, path);
const gemmi::Mtz mtz = gemmi::read_mtz_file(path);
std::filesystem::remove(path);
// HKL_base at id 0, the data at id 1. A data dataset written at id 0 occupies the id MTZ
// reserves for the base, and mtzlib then reports CU_KALPHA_A instead of the real wavelength.
REQUIRE(mtz.datasets.size() == 2);
CHECK(mtz.datasets[0].id == 0);
CHECK(mtz.datasets[0].dataset_name == "HKL_base");
CHECK(mtz.datasets[1].id == 1);
CHECK(mtz.datasets[1].wavelength == Catch::Approx(experiment.GetWavelength_A()).epsilon(1e-5));
CHECK(mtz.datasets[1].wavelength != Catch::Approx(CU_KALPHA_A).epsilon(1e-3));
// The wavelength is read off the dataset the data columns belong to, so they have to be on the
// data dataset and not on the base.
for (const char *label : {"IMEAN", "SIGIMEAN", "F", "SIGF", "FreeR_flag"}) {
const gemmi::Mtz::Column *col = mtz.column_with_label(label);
REQUIRE(col != nullptr);
CHECK(col->dataset_id == 1);
}
// Cell and space group travel in the same header.
CHECK(mtz.spacegroup != nullptr);
CHECK(mtz.spacegroup->number == 96);
CHECK(mtz.cell.a == Catch::Approx(TETRAGONAL_CELL.a).epsilon(1e-5));
CHECK(mtz.cell.c == Catch::Approx(TETRAGONAL_CELL.c).epsilon(1e-5));
CHECK(mtz.cell.gamma == Catch::Approx(90.0).epsilon(1e-5));
CHECK(mtz.datasets[1].cell.a == Catch::Approx(TETRAGONAL_CELL.a).epsilon(1e-5));
CHECK(mtz.nreflections == static_cast<int>(reflections.size()));
}
TEST_CASE("Unmerged MTZ: LP is Lorentz-polarization, QE the sensor efficiency, FLIGHT the flight path",
"[write_reflections]") {
// The whole point of the split: LP must mean what XDS and DIALS mean by it, and the raw count
// sum must still be recoverable from the file alone, as I / LP * QE * FLIGHT.
auto experiment = TestExperiment();
experiment.Goniometer(GoniometerAxis("omega", 0.0f, 0.1f, Coord(-1, 0, 0), {}));
IntegrationOutcome outcome;
const float raw[3] = {1000.0f, 250.0f, 40.0f};
const float lp[3] = {1.75f, 2.50f, 0.90f}; // Lorentz x polarization, and nothing else
const float qe[3] = {0.9375f, 0.8125f, 1.0f}; // 1.0 = the sensor said nothing to correct
const float fl[3] = {1.0125f, 1.0400f, 1.0f}; // >= 1: an oblique reflection crossed more air
for (int i = 0; i < 3; ++i) {
Reflection r{};
r.h = 4 + i; r.k = 2; r.l = 6;
r.image_number = static_cast<float>(i);
r.d = 5.0f + i;
r.I = raw[i]; // the writer is what applies the factor
r.sigma = std::sqrt(raw[i]);
r.prescaling_corr = lp[i];
r.qe_corr = qe[i];
r.flight_corr = fl[i];
r.partiality = 1.0f;
r.predicted_x = 100.0f + i; r.predicted_y = 200.0f + i;
r.observed_x = NAN; r.observed_y = NAN;
outcome.reflections.push_back(r);
}
const auto path = (std::filesystem::temp_directory_path() / "rugnux_unmerged_qe.mtz").string();
WriteUnmergedMtzReflections({outcome}, TETRAGONAL_CELL, experiment, false, path);
const gemmi::Mtz mtz = gemmi::read_mtz_file(path);
std::filesystem::remove(path);
const gemmi::Mtz::Column *c_I = mtz.column_with_label("I");
const gemmi::Mtz::Column *c_lp = mtz.column_with_label("LP");
const gemmi::Mtz::Column *c_qe = mtz.column_with_label("QE");
const gemmi::Mtz::Column *c_fl = mtz.column_with_label("FLIGHT");
REQUIRE(c_I != nullptr);
REQUIRE(c_lp != nullptr);
REQUIRE(c_qe != nullptr); // DIALS writes this column even when there is nothing in it
REQUIRE(c_fl != nullptr);
REQUIRE(mtz.nreflections == 3);
for (int i = 0; i < 3; ++i) {
const float I = mtz.data[i * mtz.columns.size() + c_I->idx];
const float LP = mtz.data[i * mtz.columns.size() + c_lp->idx];
const float QE = mtz.data[i * mtz.columns.size() + c_qe->idx];
const float FL = mtz.data[i * mtz.columns.size() + c_fl->idx];
INFO("row " << i);
// LP holds Lorentz x polarization alone: the sensor term was never inside it.
CHECK(LP == Catch::Approx(lp[i]).epsilon(1e-5));
// QE is a divisor normalised to 1 at normal incidence, so it never drops below 1.
CHECK(QE == Catch::Approx(1.0f / qe[i]).epsilon(1e-5));
CHECK(QE >= 1.0f);
// FLIGHT is a divisor in the same convention, and runs the other way: the sensor favours an
// oblique reflection, the medium attenuates it, so this one never rises above 1.
CHECK(FL == Catch::Approx(1.0f / fl[i]).epsilon(1e-5));
CHECK(FL <= 1.0f);
// ... and the three together put the raw counts back.
CHECK(I / LP * QE * FL == Catch::Approx(raw[i]).epsilon(1e-4));
// The intensity itself is the fully corrected value - all three applied.
CHECK(I == Catch::Approx(raw[i] * lp[i] * qe[i] * fl[i]).epsilon(1e-5));
}
}