A reflection the group predicts absent counted as a violation when
I/sigma > 3 AND E^2 = I/<I>(shell) > 0.3. Neither half survives contact
with real data:
* merged sigma is floored at b|I|, so merged I/sigma saturates at ISa
for nearly every reflection - the I/sigma half is an on/off switch
keyed on ISa vs 3, not a per-reflection test. On one crystal the
absent class read <I/s> 4.10 against 3.73 for the present class while
being genuinely extinct;
* <I>(shell) decays with resolution while a systematically-absent
reflection keeps a small NON-decaying residual (background / profile
leakage), so absent reflections drift over an absolute E^2 cut at high
resolution. That cost a tetragonal 42_12 crystal its 4_1: 18 of its 47
absent 00l crossed the cut, all beyond 3.7 A, at absolute intensities
identical to the low-resolution ones correctly judged absent, while
their l=4n row-mates sat 20-60x higher at the same resolution.
A screw extinguishes only the reflections that lie ON its axis, so the
fair yardstick is the rest of that same row. The threshold is now
0.3 * max(1, median E^2 of the reflection's own row), the row being the
gcd-reduced reciprocal-space direction and the control class the same-row
reflections the group predicts present. Floored at 1, so it only ever
relaxes: a screw can be recovered by it, never lost.
Per row, not pooled. A 4_1 along c and a 2_1 along a are separate
conditions with separate controls; pooling let the weak a/b rows (median
E^2 ~0.5) set the threshold for a strong c row (8.4) and the rescue never
fired.
The candidate table now reports the screw evidence (median E^2 of the
absent class and of its rows) - the <I/s> columns are the centering
evidence and say nothing about screws, for the sigma-floor reason above.
Rotation battery, 33 crystals: 31 decisions bit-identical, the 42_12
crystal recovers its 4_1 (0 violations, row E^2 8.4 vs absent 0.12), and
one crystal with a long axis and heavy 00l overlap moves to a 4_1 group at
exactly 10.0% violations - marginal, and its sister crystal of the same
form sits at 13.3% and does not move. Real screws now span 0-9.3%
violations, so max_absent_violation_fraction cannot be tightened below
0.10 without risking a genuine one.
Co-Authored-By: Claude Opus 5 (1M context) <noreply@anthropic.com>
237 lines
9.3 KiB
C++
237 lines
9.3 KiB
C++
#include <catch2/catch_all.hpp>
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#include "../image_analysis/scale_merge/SearchSpaceGroup.h"
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#include "gemmi/symmetry.hpp"
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#include <algorithm>
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#include <cmath>
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#include <cstdint>
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#include <string>
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#include <tuple>
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#include <unordered_set>
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#include <vector>
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namespace {
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struct HKL {
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int h = 0;
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int k = 0;
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int l = 0;
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bool operator==(const HKL& o) const noexcept {
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return h == o.h && k == o.k && l == o.l;
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}
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};
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struct HKLHash {
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size_t operator()(const HKL& x) const noexcept {
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auto mix = [](uint64_t v) {
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v ^= v >> 33;
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v *= 0xff51afd7ed558ccdULL;
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v ^= v >> 33;
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v *= 0xc4ceb9fe1a85ec53ULL;
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v ^= v >> 33;
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return v;
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};
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return static_cast<size_t>(
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mix(static_cast<uint64_t>(x.h)) ^
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(mix(static_cast<uint64_t>(x.k)) << 1) ^
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(mix(static_cast<uint64_t>(x.l)) << 2));
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}
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};
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double CalcSyntheticD(int h, int k, int l) {
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const double q2 = static_cast<double>(h * h + k * k + l * l);
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return 40.0 / std::sqrt(q2 + 1.0);
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}
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double SyntheticIntensityFromAsu(const gemmi::Op::Miller& asu) {
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uint64_t x = static_cast<uint64_t>((asu[0] + 31) * 73856093u) ^
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static_cast<uint64_t>((asu[1] + 37) * 19349663u) ^
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static_cast<uint64_t>((asu[2] + 41) * 83492791u);
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x ^= x >> 13;
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x *= 0x9e3779b97f4a7c15ULL;
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x ^= x >> 17;
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return 100.0 + static_cast<double>(x % 500);
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}
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std::vector<MergedReflection> GenerateMergedReflectionsForSpaceGroup(
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const gemmi::SpaceGroup& sg,
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int hmax = 8) {
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std::vector<MergedReflection> merged;
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std::unordered_set<HKL, HKLHash> added;
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const gemmi::GroupOps gops = sg.operations();
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const gemmi::ReciprocalAsu rasu(&sg);
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for (int h = -hmax; h <= hmax; ++h) {
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for (int k = -hmax; k <= hmax; ++k) {
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for (int l = -hmax; l <= hmax; ++l) {
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if (h == 0 && k == 0 && l == 0)
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continue;
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bool absent = false;
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gemmi::Op::Miller hkl{{h, k, l}};
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if (gops.is_systematically_absent(hkl))
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absent = true;
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const auto [asu, sign_plus] = rasu.to_asu_sign(hkl, gops);
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if (!sign_plus)
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continue;
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const HKL key{h, k, l};
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if (added.find(key) != added.end())
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continue;
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added.insert(key);
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merged.push_back(MergedReflection{
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.h = h,
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.k = k,
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.l = l,
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.I = absent ? 0.0 : SyntheticIntensityFromAsu(asu),
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.sigma = 1.0,
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.d = CalcSyntheticD(h, k, l)
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});
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}
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}
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}
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return merged;
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}
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}
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TEST_CASE("SearchSpaceGroup detects synthetic space groups") {
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struct Case {
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std::string input_name;
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std::string expected_short_name;
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};
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const std::vector<Case> cases = {
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{"P 1", "P1"},
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{"P 1 2 1", "P2"},
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{"P 3 2 1", "P321"},
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{"P 4 2 2", "P422"},
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{"P 4 3 2", "P432"},
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{"P 43 21 2", "P43212"},
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{"P 6 2 2", "P622"},
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{"C 1 2 1", "C2"},
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{"C 2 2 2", "C222"},
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{"I 4 3 2", "I432"},
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{"I 21 21 21", "I212121"},
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{"I 2 1 3", "I213"},
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};
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for (const auto& tc : cases) {
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DYNAMIC_SECTION(tc.expected_short_name) {
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const gemmi::SpaceGroup& sg = gemmi::get_spacegroup_by_name(tc.input_name);
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const auto merged = GenerateMergedReflectionsForSpaceGroup(sg);
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SearchSpaceGroupOptions opt;
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opt.merge_friedel = true;
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const auto result = SearchSpaceGroup(merged, opt);
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// Several inputs cannot be told apart from intensities alone: enantiomorphic partners
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// (P4_3 vs P4_1) and origin-ambiguous pairs (I2_12_12_1 vs I222, I2_13 vs I2_3) share
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// the same systematic absences. The search reports those as alternatives, so the
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// expected group must appear among the best group and its alternatives.
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std::vector<std::string> accepted;
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if (result.best_space_group.has_value())
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accepted.push_back(result.best_space_group->short_name());
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for (const auto& alt : result.alternatives)
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accepted.push_back(alt.short_name());
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INFO(SearchSpaceGroupResultToText(result));
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REQUIRE(result.best_space_group.has_value());
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CHECK(std::find(accepted.begin(), accepted.end(), tc.expected_short_name) != accepted.end());
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}
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}
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}
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// Regression: a real screw axis whose systematically-absent reflections carry a genuinely weak
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// intensity but an UNDER-estimated sigma (so their I/sigma clears the "present" cut) must still be
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// found. Reproduces a monoclinic 2_1 miss on weakly-diffracting monoclinic data, where the merged sigmas on
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// the 0k0-odd reflections were ~2x too small and faked screw-axis violations. The E^2 intensity gate
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// (present_e_squared) is what keeps those reflections classified absent.
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TEST_CASE("SearchSpaceGroup finds a screw axis despite under-estimated sigmas on absent reflections") {
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const gemmi::SpaceGroup& sg = gemmi::get_spacegroup_by_name("P 1 21 1");
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auto merged = GenerateMergedReflectionsForSpaceGroup(sg, 18);
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// Every systematically-absent (0k0, k odd) reflection: small-but-nonzero intensity (~2% of a
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// normal reflection) with a far-too-small sigma, so I/sigma ~ 27 fakes a "present" reflection.
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const gemmi::GroupOps gops = sg.operations();
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int absent_count = 0;
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for (auto& r : merged) {
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const gemmi::Op::Miller hkl{{r.h, r.k, r.l}};
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if (gops.is_systematically_absent(hkl)) {
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r.I = 8.0f;
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r.sigma = 0.3f;
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++absent_count;
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}
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}
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REQUIRE(absent_count >= 8); // enough predicted-absent reflections to be trusted
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SearchSpaceGroupOptions opt;
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opt.merge_friedel = true;
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SECTION("intensity gate on (default): screw recovered") {
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const auto result = SearchSpaceGroup(merged, opt);
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INFO(SearchSpaceGroupResultToText(result));
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REQUIRE(result.best_space_group.has_value());
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CHECK(result.best_space_group->short_name() == "P21");
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}
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SECTION("intensity gate off (I/sigma only): the screw is missed") {
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// Documents the failure the gate fixes: with I/sigma alone the too-small sigmas fake
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// violations and the search falls back to the symmorphic group.
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opt.present_e_squared = 0.0;
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const auto result = SearchSpaceGroup(merged, opt);
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INFO(SearchSpaceGroupResultToText(result));
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REQUIRE(result.best_space_group.has_value());
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CHECK(result.best_space_group->short_name() == "P2");
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}
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}
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// Regression: the E^2 gate above compares a reflection to the mean of its RESOLUTION SHELL, which
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// falls off with resolution, while a systematically-absent reflection keeps a small non-decaying
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// residual (background / profile leakage). On a crystal whose axial rows are much stronger than an
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// average reflection, that turns the high-resolution residuals into screw-axis violations and the
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// screw is lost, although the reflections beside them in the same row are tens of times stronger.
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// A tetragonal 42_12 case failed exactly this way (18 of 47 absent 00l over the cut, all beyond
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// 3.7 A, at 1-2% of the l=4n reflections next to them). The threshold is therefore taken relative to
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// the axial row the screw constrains, not to the shell.
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TEST_CASE("SearchSpaceGroup finds a screw axis whose absent class is weak only within its own row") {
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const gemmi::SpaceGroup& sg = gemmi::get_spacegroup_by_name("P 43 21 2");
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auto merged = GenerateMergedReflectionsForSpaceGroup(sg, 12);
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// Axial rows 40x stronger than a general reflection, and an absent class carrying ~2% of its own
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// row - but half of a general reflection, so a threshold set against the shell calls every one of
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// them a violation while a threshold set against the row calls none.
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const gemmi::GroupOps gops = sg.operations();
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int absent_on_axis = 0;
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for (auto& r : merged) {
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const gemmi::Op::Miller hkl{{r.h, r.k, r.l}};
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if (gops.epsilon_factor_without_centering(hkl) <= 1)
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continue;
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if (gops.is_systematically_absent(hkl)) {
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r.I = 300.0f;
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r.sigma = 1.0f;
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++absent_on_axis;
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} else {
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r.I *= 40.0f;
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}
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}
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REQUIRE(absent_on_axis >= 8);
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SearchSpaceGroupOptions opt;
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opt.merge_friedel = true;
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const auto result = SearchSpaceGroup(merged, opt);
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INFO(SearchSpaceGroupResultToText(result));
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REQUIRE(result.best_space_group.has_value());
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// P4_1 2_1 2 and P4_3 2_1 2 are enantiomorphs and indistinguishable from intensities.
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std::vector<std::string> accepted{result.best_space_group->short_name()};
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for (const auto& alt : result.alternatives)
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accepted.push_back(alt.short_name());
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CHECK(std::find(accepted.begin(), accepted.end(), "P43212") != accepted.end());
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} |