Jungfraujoch/tests/SearchSpaceGroupTest.cpp

#include <catch2/catch_all.hpp>

#include "../image_analysis/scale_merge/SearchSpaceGroup.h"
#include "gemmi/symmetry.hpp"

#include <algorithm>
#include <cmath>
#include <cstdint>
#include <string>
#include <tuple>
#include <unordered_set>
#include <vector>

namespace {
    struct HKL {
        int h = 0;
        int k = 0;
        int l = 0;

        bool operator==(const HKL& o) const noexcept {
            return h == o.h && k == o.k && l == o.l;
        }
    };

    struct HKLHash {
        size_t operator()(const HKL& x) const noexcept {
            auto mix = [](uint64_t v) {
                v ^= v >> 33;
                v *= 0xff51afd7ed558ccdULL;
                v ^= v >> 33;
                v *= 0xc4ceb9fe1a85ec53ULL;
                v ^= v >> 33;
                return v;
            };
            return static_cast<size_t>(
                mix(static_cast<uint64_t>(x.h)) ^
                (mix(static_cast<uint64_t>(x.k)) << 1) ^
                (mix(static_cast<uint64_t>(x.l)) << 2));
        }
    };

    double CalcSyntheticD(int h, int k, int l) {
        const double q2 = static_cast<double>(h * h + k * k + l * l);
        return 40.0 / std::sqrt(q2 + 1.0);
    }

    double SyntheticIntensityFromAsu(const gemmi::Op::Miller& asu) {
        uint64_t x = static_cast<uint64_t>((asu[0] + 31) * 73856093u) ^
                     static_cast<uint64_t>((asu[1] + 37) * 19349663u) ^
                     static_cast<uint64_t>((asu[2] + 41) * 83492791u);
        x ^= x >> 13;
        x *= 0x9e3779b97f4a7c15ULL;
        x ^= x >> 17;
        return 100.0 + static_cast<double>(x % 500);
    }

    std::vector<MergedReflection> GenerateMergedReflectionsForSpaceGroup(
        const gemmi::SpaceGroup& sg,
        int hmax = 8) {

        std::vector<MergedReflection> merged;
        std::unordered_set<HKL, HKLHash> added;

        const gemmi::GroupOps gops = sg.operations();
        const gemmi::ReciprocalAsu rasu(&sg);

        for (int h = -hmax; h <= hmax; ++h) {
            for (int k = -hmax; k <= hmax; ++k) {
                for (int l = -hmax; l <= hmax; ++l) {
                    if (h == 0 && k == 0 && l == 0)
                        continue;

                    bool absent = false;
                    gemmi::Op::Miller hkl{{h, k, l}};
                    if (gops.is_systematically_absent(hkl))
                        absent = true;

                    const auto [asu, sign_plus] = rasu.to_asu_sign(hkl, gops);
                    if (!sign_plus)
                        continue;

                    const HKL key{h, k, l};
                    if (added.find(key) != added.end())
                        continue;
                    added.insert(key);

                    merged.push_back(MergedReflection{
                        .h = h,
                        .k = k,
                        .l = l,
                        .I = static_cast<float>(absent ? 0.0 : SyntheticIntensityFromAsu(asu)),
                        .sigma = 1.0,
                        .d = static_cast<float>(CalcSyntheticD(h, k, l))
                    });
                }
            }
        }

        return merged;
    }
}

TEST_CASE("SearchSpaceGroup detects synthetic space groups") {
    struct Case {
        std::string input_name;
        std::string expected_short_name;
    };

    const std::vector<Case> cases = {
        {"P 1", "P1"},
        {"P 1 2 1", "P2"},
        {"P 3 2 1", "P321"},
        {"P 4 2 2", "P422"},
        {"P 4 3 2", "P432"},
        {"P 43 21 2", "P43212"},
        {"P 6 2 2", "P622"},
        {"C 1 2 1", "C2"},
        {"C 2 2 2", "C222"},
        {"I 4 3 2", "I432"},
        {"I 21 21 21", "I212121"},
        {"I 2 1 3", "I213"},
    };

    for (const auto& tc : cases) {
        DYNAMIC_SECTION(tc.expected_short_name) {
            const gemmi::SpaceGroup& sg = gemmi::get_spacegroup_by_name(tc.input_name);
            const auto merged = GenerateMergedReflectionsForSpaceGroup(sg);

            SearchSpaceGroupOptions opt;
            opt.merge_friedel = true;

            const auto result = SearchSpaceGroup(merged, opt);

            // Several inputs cannot be told apart from intensities alone: enantiomorphic partners
            // (P4_3 vs P4_1) and origin-ambiguous pairs (I2_12_12_1 vs I222, I2_13 vs I2_3) share
            // the same systematic absences. The search reports those as alternatives, so the
            // expected group must appear among the best group and its alternatives.
            std::vector<std::string> accepted;
            if (result.best_space_group.has_value())
                accepted.push_back(result.best_space_group->short_name());
            for (const auto& alt : result.alternatives)
                accepted.push_back(alt.short_name());

            INFO(SearchSpaceGroupResultToText(result));
            REQUIRE(result.best_space_group.has_value());
            CHECK(std::find(accepted.begin(), accepted.end(), tc.expected_short_name) != accepted.end());
        }
    }
}

// Regression: a real screw axis whose systematically-absent reflections carry a genuinely weak
// intensity but an UNDER-estimated sigma (so their I/sigma clears the "present" cut) must still be
// found. Reproduces a monoclinic 2_1 miss on weakly-diffracting monoclinic data, where the merged sigmas on
// the 0k0-odd reflections were ~2x too small and faked screw-axis violations. The E^2 intensity gate
// (present_e_squared) is what keeps those reflections classified absent.
TEST_CASE("SearchSpaceGroup finds a screw axis despite under-estimated sigmas on absent reflections") {
    const gemmi::SpaceGroup& sg = gemmi::get_spacegroup_by_name("P 1 21 1");
    auto merged = GenerateMergedReflectionsForSpaceGroup(sg, 18);

    // Every systematically-absent (0k0, k odd) reflection: small-but-nonzero intensity (~2% of a
    // normal reflection) with a far-too-small sigma, so I/sigma ~ 27 fakes a "present" reflection.
    const gemmi::GroupOps gops = sg.operations();
    int absent_count = 0;
    for (auto& r : merged) {
        const gemmi::Op::Miller hkl{{r.h, r.k, r.l}};
        if (gops.is_systematically_absent(hkl)) {
            r.I = 8.0f;
            r.sigma = 0.3f;
            ++absent_count;
        }
    }
    REQUIRE(absent_count >= 8);   // enough predicted-absent reflections to be trusted

    SearchSpaceGroupOptions opt;
    opt.merge_friedel = true;

    SECTION("intensity gate on (default): screw recovered") {
        const auto result = SearchSpaceGroup(merged, opt);
        INFO(SearchSpaceGroupResultToText(result));
        REQUIRE(result.best_space_group.has_value());
        CHECK(result.best_space_group->short_name() == "P21");
    }

    SECTION("intensity gate off (I/sigma only): the deferral recovers the screw anyway") {
        // This section used to document the failure the E^2 gate fixes - with I/sigma alone the
        // too-small sigmas fake violations and the search fell back to the symmorphic group. There
        // are now TWO independent defences and the second one holds here without the first: the
        // fabricated violations are still counted, but the absent class sits at 2% of its own row,
        // so the zone is dead per reflection and carries no measured pseudo-translation, which is
        // what licenses the absence evidence to override the count.
        //
        // Kept rather than deleted, because it pins the two apart: if a future change makes this
        // read P2 again, the deferral has stopped licensing a zone that is genuinely extinct.
        opt.present_e_squared = 0.0;
        const auto result = SearchSpaceGroup(merged, opt);
        INFO(SearchSpaceGroupResultToText(result));
        REQUIRE(result.best_space_group.has_value());
        CHECK(result.best_space_group->short_name() == "P21");
    }
}

// Regression: the E^2 gate above compares a reflection to the mean of its RESOLUTION SHELL, which
// falls off with resolution, while a systematically-absent reflection keeps a small non-decaying
// residual (background / profile leakage). On a crystal whose axial rows are much stronger than an
// average reflection, that turns the high-resolution residuals into screw-axis violations and the
// screw is lost, although the reflections beside them in the same row are tens of times stronger.
// A tetragonal 42_12 case failed exactly this way (18 of 47 absent 00l over the cut, all beyond
// 3.7 A, at 1-2% of the l=4n reflections next to them). The threshold is therefore taken relative to
// the axial row the screw constrains, not to the shell.
TEST_CASE("SearchSpaceGroup finds a screw axis whose absent class is weak only within its own row") {
    const gemmi::SpaceGroup& sg = gemmi::get_spacegroup_by_name("P 43 21 2");
    auto merged = GenerateMergedReflectionsForSpaceGroup(sg, 12);

    // Axial rows 40x stronger than a general reflection, and an absent class carrying ~2% of its own
    // row - but half of a general reflection, so a threshold set against the shell calls every one of
    // them a violation while a threshold set against the row calls none.
    const gemmi::GroupOps gops = sg.operations();
    int absent_on_axis = 0;
    for (auto& r : merged) {
        const gemmi::Op::Miller hkl{{r.h, r.k, r.l}};
        if (gops.epsilon_factor_without_centering(hkl) <= 1)
            continue;
        if (gops.is_systematically_absent(hkl)) {
            r.I = 300.0f;
            r.sigma = 1.0f;
            ++absent_on_axis;
        } else {
            r.I *= 40.0f;
        }
    }
    REQUIRE(absent_on_axis >= 8);

    SearchSpaceGroupOptions opt;
    opt.merge_friedel = true;

    const auto result = SearchSpaceGroup(merged, opt);
    INFO(SearchSpaceGroupResultToText(result));
    REQUIRE(result.best_space_group.has_value());
    // P4_1 2_1 2 and P4_3 2_1 2 are enantiomorphs and indistinguishable from intensities.
    std::vector<std::string> accepted{result.best_space_group->short_name()};
    for (const auto& alt : result.alternatives)
        accepted.push_back(alt.short_name());
    CHECK(std::find(accepted.begin(), accepted.end(), "P43212") != accepted.end());
}
// Regression: a screw's predicted-absent class is one row of reciprocal space, and that row is often
// the one a rotation sweep records least - it lies near the spindle, where the blind cusp maps onto
// itself and symmetry cannot fill it in. Counting the class therefore measures the geometry of the
// sweep, not the strength of the evidence, and a count gate refused a monoclinic crystal its 2_1 for
// having six 0k0-odd reflections rather than eight, every one of them measured at a thousandth of the
// row beside them. The class is judged by ScrewZoneEvidence instead, which reads the contrast
// against the row - so few-but-decisive is accepted and many-but-marginal is not.
TEST_CASE("SearchSpaceGroup weighs a screw's absences by evidence, not by how many were recorded") {
    const gemmi::SpaceGroup& sg = gemmi::get_spacegroup_by_name("P 1 21 1");
    const gemmi::GroupOps gops = sg.operations();

    SearchSpaceGroupOptions opt;
    opt.merge_friedel = true;

    SECTION("five decisive absences, below min_absent_observed: the screw is still found") {
        auto merged = GenerateMergedReflectionsForSpaceGroup(sg, 18);
        // Keep five of the 0k0-odd reflections, at a thousandth of their row, and drop the rest - as a
        // sweep along the 2-fold does, leaving too few to satisfy a count but plenty to decide.
        int kept = 0;
        std::erase_if(merged, [&](MergedReflection& r) {
            if (!gops.is_systematically_absent(gemmi::Op::Miller{{r.h, r.k, r.l}}))
                return false;
            if (kept >= 5)
                return true;
            ++kept;
            r.I = 0.5;
            return false;
        });
        REQUIRE(kept == 5);
        REQUIRE(kept < opt.min_absent_observed);

        const auto result = SearchSpaceGroup(merged, opt);
        INFO(SearchSpaceGroupResultToText(result));
        REQUIRE(result.best_space_group.has_value());
        CHECK(result.best_space_group->short_name() == "P21");
    }

    SECTION("a uniformly weak axial row decides nothing, however many absences it holds") {
        // The whole 0k0 row badly measured: the predicted-absent reflections are weak, but so is the
        // rest of their row, so there is no contrast and no screw to claim. A violation count cannot
        // see this - nothing on the row clears an absolute cut, so it reads zero violations and, with
        // enough reflections to satisfy the count, would claim the 2_1 from no evidence at all.
        auto merged = GenerateMergedReflectionsForSpaceGroup(sg, 18);
        int absent_on_row = 0;
        for (auto& r : merged) {
            if (r.h != 0 || r.l != 0)
                continue;
            const bool absent = gops.is_systematically_absent(gemmi::Op::Miller{{r.h, r.k, r.l}});
            r.I = absent ? 4.0 : 5.0;
            absent_on_row += absent ? 1 : 0;
        }
        REQUIRE(absent_on_row >= opt.min_absent_observed);

        const auto result = SearchSpaceGroup(merged, opt);
        INFO(SearchSpaceGroupResultToText(result));
        REQUIRE(result.best_space_group.has_value());
        CHECK(result.best_space_group->short_name() == "P2");
    }
}

// The operator correlation is on resolution-normalised E^2, not on raw I (see SearchSpaceGroup.cpp).
// Both members of a symmetry pair sit at the same |s|, so on raw intensities the resolution fall-off
// is variance shared perfectly between the two arms of every pair and reads as a correlation for ANY
// pairing at all. These two cases pin that down from both sides.
TEST_CASE("SearchSpaceGroup operator correlation reads symmetry, not the resolution fall-off",
          "[SearchSpaceGroup]") {
    // Intensities that are a smooth function of resolution times an INDEPENDENT per-reflection
    // factor: a Wilson-like fall-off with no symmetry in it whatsoever.
    auto radial_only = [](int hmax) {
        std::vector<MergedReflection> merged;
        for (int h = -hmax; h <= hmax; ++h)
            for (int k = -hmax; k <= hmax; ++k)
                for (int l = -hmax; l <= hmax; ++l) {
                    if ((h == 0 && k == 0 && l == 0) || std::make_tuple(-h, -k, -l) < std::make_tuple(h, k, l))
                        continue;
                    const double d = CalcSyntheticD(h, k, l);
                    const double falloff = std::exp(-30.0 / (d * d));
                    // Deterministic, independent of any symmetry mate: reuse the hash on the raw index.
                    const double jitter = SyntheticIntensityFromAsu(gemmi::Op::Miller{{h, k, l}}) / 350.0;
                    const double I = 1.0e5 * falloff * jitter;
                    merged.push_back(MergedReflection{
                        .h = h, .k = k, .l = l, .I = static_cast<float>(I),
                        .sigma = static_cast<float>(I / 20.0), .d = static_cast<float>(d)});
                }
        return merged;
    };

    SearchSpaceGroupOptions opt;
    opt.merge_friedel = true;

    SECTION("a fall-off with no symmetry in it confirms no operator") {
        const auto result = SearchSpaceGroup(radial_only(8), opt);
        INFO(SearchSpaceGroupResultToText(result));
        REQUIRE(result.operator_scores.size() > 1);
        for (const auto& s : result.operator_scores) {
            INFO("operator " << s.op_triplet_hkl);
            CHECK(s.n_pairs >= opt.min_pairs_per_operator);
            CHECK(s.cc < opt.min_operator_cc);
            CHECK_FALSE(s.present);
        }
        CHECK(result.point_group_hm == "1");
    }

    SECTION("a real operator under the same fall-off is confirmed, and does not move with the cut") {
        // Same fall-off, but the intensities now carry a genuine monoclinic 2-fold.
        const gemmi::SpaceGroup& sg = gemmi::get_spacegroup_by_name("P 1 2 1");
        const gemmi::ReciprocalAsu rasu(&sg);
        const gemmi::GroupOps gops = sg.operations();
        auto merged = radial_only(8);
        for (auto& r : merged) {
            const auto [asu, plus] = rasu.to_asu_sign(gemmi::Op::Miller{{r.h, r.k, r.l}}, gops);
            const double falloff = std::exp(-30.0 / (r.d * r.d));
            r.I = 1.0e5 * falloff * SyntheticIntensityFromAsu(asu) / 350.0;
            r.sigma = r.I / 20.0;
        }
        auto two_fold_cc = [&](double d_min) {
            SearchSpaceGroupOptions o = opt;
            o.d_min_limit_A = d_min;
            const auto result = SearchSpaceGroup(merged, o);
            INFO(SearchSpaceGroupResultToText(result));
            REQUIRE(result.point_group_hm == "2");
            double cc = -2.0;
            for (const auto& s : result.operator_scores)
                if (s.present)
                    cc = s.cc;
            REQUIRE(cc > opt.min_operator_cc);
            return cc;
        };
        // The whole point of normalising: how much of the fall-off is inside the merge no longer
        // moves the operator's score, so the search resolution cut cannot decide the symmetry.
        CHECK(std::fabs(two_fold_cc(0.0) - two_fold_cc(6.0)) < 0.05);
    }
}

// The enumeration reaches the settings gemmi does not call the reference one, and only when the cell
// has the axes they name. Both halves are pinned here: `P 1 1 2_1` puts its 2-fold and its screw on
// c, which no reference setting can express (Stage A never offers the rotation and Stage B never
// offers the group), so without the two options the answer is P1; with them, and with a cell whose
// unique axis IS c, it is named; and with a cell whose unique axis is b the same candidate is
// refused rather than adopted on axes the crystal does not have.
TEST_CASE("SearchSpaceGroup names a non-reference setting only on a cell that hosts it") {
    const gemmi::SpaceGroup& sg = gemmi::get_spacegroup_by_name("P 1 1 21");
    const auto merged = GenerateMergedReflectionsForSpaceGroup(sg, 12);

    SearchSpaceGroupOptions opt;
    opt.merge_friedel = true;

    SECTION("narrow enumeration cannot name it") {
        const auto result = SearchSpaceGroup(merged, opt);
        INFO(SearchSpaceGroupResultToText(result));
        REQUIRE(result.best_space_group.has_value());
        CHECK(result.best_space_group->number == 1);
    }

    SECTION("widened enumeration names it on a c-unique cell") {
        opt.cell = gemmi::UnitCell(40.0, 50.0, 60.0, 90.0, 90.0, 100.0);
        opt.enumerate_all_settings = true;
        opt.enumerate_all_rotation_sets = true;
        const auto result = SearchSpaceGroup(merged, opt);
        INFO(SearchSpaceGroupResultToText(result));
        REQUIRE(result.best_space_group.has_value());
        CHECK(result.best_space_group->xhm() == "P 1 1 21");
    }

    SECTION("a b-unique cell refuses it") {
        opt.cell = gemmi::UnitCell(40.0, 50.0, 60.0, 90.0, 100.0, 90.0);
        opt.enumerate_all_settings = true;
        opt.enumerate_all_rotation_sets = true;
        const auto result = SearchSpaceGroup(merged, opt);
        INFO(SearchSpaceGroupResultToText(result));
        REQUIRE(result.best_space_group.has_value());
        CHECK(result.best_space_group->number == 1);
    }
}

// The screw axes of an orthorhombic crystal can lie on any pair of axes, and only one of the three
// namings of #18 is a reference setting. With the narrow enumeration the group that predicts a
// SUBSET of the real absences and nothing else wins on no evidence at all, so the reported group is
// wrong rather than low - the widening is what makes the correct one available.
TEST_CASE("SearchSpaceGroup names an orthorhombic screw pair on the axes it lies on") {
    const gemmi::SpaceGroup& sg = gemmi::get_spacegroup_by_name("P 2 21 21");
    const auto merged = GenerateMergedReflectionsForSpaceGroup(sg, 14);

    SearchSpaceGroupOptions opt;
    opt.merge_friedel = true;
    opt.lattice_system = gemmi::CrystalSystem::Orthorhombic;

    SECTION("narrow enumeration reports the wrong group") {
        const auto result = SearchSpaceGroup(merged, opt);
        INFO(SearchSpaceGroupResultToText(result));
        REQUIRE(result.best_space_group.has_value());
        CHECK(result.best_space_group->number != 18);
    }

    SECTION("widened enumeration reports it") {
        opt.cell = gemmi::UnitCell(40.0, 50.0, 60.0, 90.0, 90.0, 90.0);
        opt.enumerate_all_settings = true;
        const auto result = SearchSpaceGroup(merged, opt);
        INFO(SearchSpaceGroupResultToText(result));
        REQUIRE(result.best_space_group.has_value());
        CHECK(result.best_space_group->xhm() == "P 2 21 21");
    }
}

// The centring half of the same widening. A, B and C centring on one orthorhombic cell are three
// different lattices, and only C is a reference setting, so an A-centred crystal used to have its
// centring refused (its absent class is not the one C predicts) and came out primitive. The
// candidate is now offered, and it has to be adopted from its own absences rather than from the
// metric, which cannot tell A from C at all.
TEST_CASE("SearchSpaceGroup names an A-centred orthorhombic lattice") {
    const gemmi::SpaceGroup& sg = gemmi::get_spacegroup_by_name("A 2 2 2");
    const auto merged = GenerateMergedReflectionsForSpaceGroup(sg, 12);

    SearchSpaceGroupOptions opt;
    opt.merge_friedel = true;
    opt.lattice_system = gemmi::CrystalSystem::Orthorhombic;

    SECTION("narrow enumeration cannot name it") {
        const auto result = SearchSpaceGroup(merged, opt);
        INFO(SearchSpaceGroupResultToText(result));
        REQUIRE(result.best_space_group.has_value());
        CHECK(result.best_space_group->centring_type() != 'A');
    }

    SECTION("widened enumeration names it") {
        opt.cell = gemmi::UnitCell(40.0, 50.0, 60.0, 90.0, 90.0, 90.0);
        opt.enumerate_all_settings = true;
        const auto result = SearchSpaceGroup(merged, opt);
        INFO(SearchSpaceGroupResultToText(result));
        REQUIRE(result.best_space_group.has_value());
        CHECK(result.best_space_group->xhm() == "A 2 2 2");
    }
}

// The null the widening has to survive. Stage A's second pass offers the a- and c-unique 2-folds on
// any metric that could host them, which is every orthorhombic one - so a genuinely triclinic
// crystal sitting on a pseudo-orthorhombic cell is now offered three promotions where it used to be
// offered one. It must still be refused all three: the added candidates go through the same operator
// correlation as every other, and a rotation the intensities do not have scores nothing.
TEST_CASE("SearchSpaceGroup does not promote triclinic data on a pseudo-orthorhombic cell") {
    const gemmi::SpaceGroup& sg = gemmi::get_spacegroup_by_name("P 1");
    const auto merged = GenerateMergedReflectionsForSpaceGroup(sg, 10);

    SearchSpaceGroupOptions opt;
    opt.merge_friedel = true;
    opt.lattice_system = gemmi::CrystalSystem::Orthorhombic;
    opt.cell = gemmi::UnitCell(40.0, 50.0, 60.0, 90.0, 90.0, 90.0);
    opt.enumerate_all_settings = true;
    opt.enumerate_all_rotation_sets = true;

    const auto result = SearchSpaceGroup(merged, opt);
    INFO(SearchSpaceGroupResultToText(result));
    REQUIRE(result.best_space_group.has_value());
    CHECK(result.best_space_group->number == 1);
    CHECK(result.point_group_order == 1);
}

// A zone whose predicted absences were never measurable must not outscore a zone that is genuinely
// dead. sum_u is a sum of max(0, E^2)/row_mean, so it is EXACTLY zero when every absent reflection in
// the zone merged non-positive - and the Beta tail then diverges, worth ~690 nats per reflection. That
// was harmless while the number only had to clear a bound; it is now summed across zones and ranks the
// candidates, so it made a candidate claiming a screw on an UNMEASURED row beat one whose rows are
// actually dead. The evidence is scored through the same entry point for both kinds of absence.
TEST_CASE("AbsenceEvidence does not reward a zone that was never measurable", "[SearchSpaceGroup]") {
    // 2 absences that all merged non-positive, against a control of 8...
    const double unmeasurable = AbsenceEvidence(0.0, 2, 8);
    // ...against a genuinely dead zone: 6 absences at 1% of their row's mean, same control.
    const double genuine = AbsenceEvidence(0.06, 6, 8);

    CHECK(std::isfinite(unmeasurable));
    CHECK(unmeasurable < genuine);                 // the ordering that was inverted
    CHECK(unmeasurable < 20.0);                    // and it does not clear min_screw_absence_evidence

    // The floor is far below any real measurement, so a genuine zone is untouched by it.
    CHECK(genuine == Catch::Approx(22.0).margin(0.2));
    CHECK(AbsenceEvidence(0.22, 22, 8) == Catch::Approx(65.4).margin(0.3));

    // More dead reflections still means more evidence, which is the property the sum relies on.
    CHECK(AbsenceEvidence(0.0, 6, 8) > AbsenceEvidence(0.0, 2, 8));
}

// ---------------------------------------------------------------------------------------------
// Glide planes (small-molecule space groups).
//
// A glide extinguishes a two-dimensional ZONE where a screw extinguishes a row, so it is the same
// absence test on a plane. What these cases pin is not that the test works - it is the two places
// it must NOT act: on a Sohncke group (a chiral crystal has no glide, and the corpus measurement
// that licensed this feature is a zero false-positive rate on 140 protein datasets), and on an
// inversion centre (Friedel's law makes it unmeasurable, so it must never be claimed).
// ---------------------------------------------------------------------------------------------
TEST_CASE("SearchSpaceGroup names a glide plane") {
    struct Case {
        std::string input_name;
        std::string expected_xhm;
        gemmi::UnitCell cell;
    };
    const gemmi::UnitCell monoclinic(11.0, 13.0, 17.0, 90.0, 101.0, 90.0);
    const gemmi::UnitCell orthorhombic(11.0, 13.0, 17.0, 90.0, 90.0, 90.0);

    const std::vector<Case> cases = {
        // The reference setting, and the non-reference one the same group takes when the data are
        // indexed with the glide on a: a setting names the mirror by AXIS, so both have to be
        // reachable or a crystal indexed the other way round is named wrongly or not at all.
        {"P 1 21/c 1", "P 1 21/c 1", monoclinic},
        {"P 1 21/a 1", "P 1 21/a 1", monoclinic},
        {"C 1 2/c 1",  "C 1 2/c 1",  monoclinic},
        // Three glide planes at once: every zone must be dead, not just the best one.
        {"P b c a",    "P b c a",    orthorhombic},
    };

    for (const auto& tc : cases) {
        DYNAMIC_SECTION(tc.expected_xhm) {
            const gemmi::SpaceGroup& sg = gemmi::get_spacegroup_by_name(tc.input_name);
            const auto merged = GenerateMergedReflectionsForSpaceGroup(sg, 10);

            SearchSpaceGroupOptions opt;
            opt.merge_friedel = true;
            opt.cell = tc.cell;
            opt.enumerate_all_settings = true;

            const auto result = SearchSpaceGroup(merged, opt);
            INFO(SearchSpaceGroupResultToText(result));
            REQUIRE(result.best_space_group.has_value());
            CHECK(result.best_space_group->xhm() == tc.expected_xhm);
            // The Sohncke answer is reported alongside on the same run, so a reader who knows the
            // sample is chiral never has to process the images again to see it.
            CHECK(result.sohncke_space_group.has_value());
            CHECK(result.sohncke_space_group->is_sohncke());
            REQUIRE_FALSE(result.glide_zones.empty());
            for (const auto& z : result.glide_zones)
                CHECK(z.evidence_per_reflection >= opt.min_glide_evidence_per_reflection);
        }
    }
}

// The inert direction, which is the one that matters: a chiral crystal has no glide plane, so on
// Sohncke data the glide machinery must add nothing at all - not a different group, not a zone.
TEST_CASE("SearchSpaceGroup claims no glide on Sohncke data") {
    const gemmi::UnitCell monoclinic(11.0, 13.0, 17.0, 90.0, 101.0, 90.0);
    for (const std::string name : {"P 1 21 1", "P 1 2 1", "C 1 2 1"}) {
        DYNAMIC_SECTION(name) {
            const gemmi::SpaceGroup& sg = gemmi::get_spacegroup_by_name(name);
            const auto merged = GenerateMergedReflectionsForSpaceGroup(sg, 10);

            SearchSpaceGroupOptions opt;
            opt.merge_friedel = true;
            opt.cell = monoclinic;
            opt.enumerate_all_settings = true;

            const auto result = SearchSpaceGroup(merged, opt);
            INFO(SearchSpaceGroupResultToText(result));
            REQUIRE(result.best_space_group.has_value());
            CHECK(result.best_space_group->is_sohncke());
            CHECK_FALSE(result.glide_space_group.has_value());
            CHECK(result.glide_zones.empty());
        }
    }
}

// The centre of symmetry is NOT determinable and must never be claimed: Friedel's law makes the
// diffraction pattern centrosymmetric whether or not the crystal is, so P 1 2/m 1 predicts exactly
// what P 1 2 1 predicts. Data generated in the centrosymmetric group must still come out Sohncke -
// which is the enumeration refusing any non-Sohncke group whose absences a Sohncke one already has.
TEST_CASE("SearchSpaceGroup never claims an inversion centre") {
    const gemmi::UnitCell monoclinic(11.0, 13.0, 17.0, 90.0, 101.0, 90.0);
    const gemmi::SpaceGroup& sg = gemmi::get_spacegroup_by_name("P 1 2/m 1");
    const auto merged = GenerateMergedReflectionsForSpaceGroup(sg, 10);

    SearchSpaceGroupOptions opt;
    opt.merge_friedel = true;
    opt.cell = monoclinic;
    opt.enumerate_all_settings = true;

    const auto result = SearchSpaceGroup(merged, opt);
    INFO(SearchSpaceGroupResultToText(result));
    REQUIRE(result.best_space_group.has_value());
    CHECK(result.best_space_group->is_sohncke());
    CHECK_FALSE(result.glide_space_group.has_value());
}