gam-sae 0.3.155

#![cfg(test)]
// Split from tests.rs under the #780 oversized-file gate: recovery-suite +
// registry/assignment tests from line ~6560 onward. Shared fixtures come via
// the parent-module glob below.
//
// `manifold/mod.rs` declares this module only as `#[cfg(test)] mod
// tests_recovery_split_780;`, and this attribute states that test-only scope in
// the file itself — a claim the compiler enforces rather than one carried by
// the filename.
#![cfg(test)]

use super::*;
use gam_solve::arrow_schur::{
    ArrowFactorSlab, ArrowHtbetaCache, ArrowPcgDiagnostics, ArrowSolverMode, ArrowUndampedFactors,
};
use ndarray::array;

/// Torus T^2 fit on synthetic data with a known two-frequency signal.
/// Drives a single torus atom through the [`SaeManifoldTerm`] Newton loop
/// and checks that the in-sample reconstruction R² clears 0.5.
#[test]
pub(crate) fn sae_torus_atom_recovers_two_frequency_synthetic() {
    let n = 96usize;
    let p = 4usize;
    let h = 3usize;
    let d = 2usize;
    let evaluator = TorusHarmonicEvaluator::new(d, h).unwrap();
    let m = evaluator.basis_size();
    // True coords on T^2 (phase in [0, 1)).
    let mut true_coords = Array2::<f64>::zeros((n, d));
    for i in 0..n {
        true_coords[[i, 0]] = ((i as f64) * 0.137).rem_euclid(1.0);
        true_coords[[i, 1]] = ((i as f64) * 0.241 + 0.13).rem_euclid(1.0);
    }
    // Synthetic target: a low-frequency periodic signal on T^2 mixed
    // linearly into a p-dim ambient.
    let mut z = Array2::<f64>::zeros((n, p));
    for i in 0..n {
        let t1 = 2.0 * std::f64::consts::PI * true_coords[[i, 0]];
        let t2 = 2.0 * std::f64::consts::PI * true_coords[[i, 1]];
        z[[i, 0]] = t1.sin() + 0.3 * t2.cos();
        z[[i, 1]] = t1.cos() + 0.2 * (t1 + t2).sin();
        z[[i, 2]] = t2.sin();
        z[[i, 3]] = 0.5 * (t1 - t2).cos();
    }
    let sst: f64 = z.iter().map(|v| v * v).sum::<f64>();
    // Initialise from the true coords (this test exercises basis correctness
    // and decoder fit, not coordinate identification on T^2).
    let (phi0, jet0) = evaluator.evaluate(true_coords.view()).unwrap();
    // Penalty: identity-on-non-constant + tiny floor on constant.
    let mut penalty = Array2::<f64>::eye(m);
    penalty *= 1.0e-4;
    let atom = SaeManifoldAtom::new_with_provided_function_gram(
        "torus_atom",
        SaeAtomBasisKind::Torus,
        d,
        phi0,
        jet0,
        Array2::<f64>::zeros((m, p)),
        penalty,
    )
    .unwrap()
    .with_basis_evaluator(Arc::new(TorusHarmonicEvaluator::new(d, h).unwrap()));

    let assignment = SaeAssignment::from_blocks_with_mode_and_manifolds(
        Array2::<f64>::zeros((n, 1)),
        vec![true_coords],
        vec![LatentManifold::Product(vec![
            LatentManifold::Circle { period: 1.0 },
            LatentManifold::Circle { period: 1.0 },
        ])],
        AssignmentMode::softmax(0.5),
    )
    .unwrap();
    let mut term = SaeManifoldTerm::new(vec![atom], assignment).unwrap();
    // ARD log-precision is per-axis (length == atom latent dim), not a
    // single scalar — see `SaeManifoldRho::to_flat` / `from_flat` and
    // the validation in `negative_log_ard_prior` (`ARD rho atom k has
    // len ... but atom dim is d`).
    let mut rho = SaeManifoldRho::new(0.0, -4.0, vec![Array1::<f64>::zeros(d)]);
    let ridge = 1.0e-6;
    for _ in 0..10 {
        let loss = term
            .run_joint_fit_arrow_schur(z.view(), &mut rho, None, 1, 1.0, ridge, ridge)
            .unwrap();
        if !loss.total().is_finite() {
            break;
        }
    }
    let fitted = term.fitted();
    assert_eq!(fitted.dim(), (n, p));
    let mut sse = 0.0_f64;
    for ((row, col), v) in fitted.indexed_iter() {
        let r = v - z[[row, col]];
        sse += r * r;
    }
    let r2 = 1.0 - sse / sst.max(1.0e-12);
    assert!(
        r2 >= 0.5,
        "torus atom R² too low: {r2:.4} (sst={sst:.4}, sse={sse:.4})"
    );
}

/// Sphere S² fit on a synthetic spherical signal. Drives a single sphere
/// atom through the [`SaeManifoldTerm`] Newton loop and checks in-sample
/// R² ≥ 0.5.
#[test]
pub(crate) fn sae_sphere_atom_recovers_synthetic_signal() {
    let n = 96usize;
    let p = 3usize;
    // Ambient coordinate width: `S²` is intrinsically 2-D but carried as a unit
    // 3-vector.
    let d = 3usize;
    // A spiral of true directions. The generating (lat, lon) is a convenient way
    // to trace one, but the COORDINATE is the direction it names.
    let mut true_coords = Array2::<f64>::zeros((n, d));
    let mut z = Array2::<f64>::zeros((n, p));
    for i in 0..n {
        let t = (i as f64) / (n as f64);
        let lat = -0.5 + 1.0 * t;
        let lon = -std::f64::consts::PI + 2.0 * std::f64::consts::PI * t;
        let (x, y, zc) = (lat.cos() * lon.cos(), lat.cos() * lon.sin(), lat.sin());
        true_coords[[i, 0]] = x;
        true_coords[[i, 1]] = y;
        true_coords[[i, 2]] = zc;
        z[[i, 0]] = x;
        z[[i, 1]] = y;
        z[[i, 2]] = zc;
    }
    let sst: f64 = z.iter().map(|v| v * v).sum::<f64>();
    let (phi0, jet0) = AmbientSphereHarmonicEvaluator::new(2)
        .unwrap()
        .evaluate(true_coords.view()).unwrap();
    let m = phi0.ncols();
    let mut penalty = Array2::<f64>::eye(m);
    penalty *= 1.0e-4;
    let atom = SaeManifoldAtom::new_with_provided_function_gram(
        "sphere_atom",
        SaeAtomBasisKind::Sphere,
        d,
        phi0,
        jet0,
        Array2::<f64>::zeros((m, p)),
        penalty,
    )
    .unwrap()
    .with_basis_evaluator(Arc::new(AmbientSphereHarmonicEvaluator::new(2).unwrap()));

    let assignment = SaeAssignment::from_blocks_with_mode_and_manifolds(
        Array2::<f64>::zeros((n, 1)),
        vec![true_coords],
        vec![LatentManifold::Sphere { dim: 3 }],
        AssignmentMode::softmax(0.5),
    )
    .unwrap();
    let mut term = SaeManifoldTerm::new(vec![atom], assignment).unwrap();
    // The sphere atom's coordinate is a 3-wide ambient vector, so per-axis ARD
    // carries one log-precision per AMBIENT axis. A shorter block would be
    // indexed out of bounds in the per-axis assembly loop and is rejected by
    // the per-axis ARD contract.
    let mut rho = SaeManifoldRho::new(0.0, -4.0, vec![Array1::<f64>::zeros(3)]);
    let ridge = 1.0e-6;
    for _ in 0..10 {
        let loss = term
            .run_joint_fit_arrow_schur(z.view(), &mut rho, None, 1, 1.0, ridge, ridge)
            .unwrap();
        if !loss.total().is_finite() {
            break;
        }
    }
    let fitted = term.fitted();
    assert_eq!(fitted.dim(), (n, p));
    let mut sse = 0.0_f64;
    for ((row, col), v) in fitted.indexed_iter() {
        let r = v - z[[row, col]];
        sse += r * r;
    }
    let r2 = 1.0 - sse / sst.max(1.0e-12);
    assert!(
        r2 >= 0.5,
        "sphere atom R² too low: {r2:.4} (sst={sst:.4}, sse={sse:.4})"
    );
}

/// Mirror of the Python `test_sae_manifold_softmax_dispatch` shape: drive a
/// single periodic atom on a 1-harmonic synthetic target with 10 Newton
/// steps end-to-end in Rust and check that the multi-step loop achieves
/// in-sample R² ≥ 0.95.
#[test]
pub(crate) fn sae_manifold_fit_10_steps_one_harmonic_reaches_high_r2() {
    let n = 64usize;
    let m = 3usize;
    let p = 1usize;

    let true_t: Vec<f64> = (0..n).map(|i| (i as f64) / (n as f64)).collect();
    let mut z = Array2::<f64>::zeros((n, p));
    for i in 0..n {
        let angle = 2.0 * std::f64::consts::PI * true_t[i];
        z[[i, 0]] = 0.7 * angle.sin() + 0.3 * angle.cos();
    }
    let sst: f64 = z.iter().map(|v| v * v).sum::<f64>();

    let evaluator = PeriodicHarmonicEvaluator::new(m).unwrap();
    let mut coords0_data = Array2::<f64>::zeros((n, 1));
    for i in 0..n {
        // Phase-shifted initialization so the optimizer must do real work.
        coords0_data[[i, 0]] = (true_t[i] + 0.25).rem_euclid(1.0);
    }
    let (phi0, jet0) = evaluator.evaluate(coords0_data.view()).unwrap();

    let atom = SaeManifoldAtom::new_with_provided_function_gram(
        "periodic_atom",
        SaeAtomBasisKind::Periodic,
        1,
        phi0,
        jet0,
        Array2::<f64>::zeros((m, p)),
        Array2::<f64>::eye(m),
    )
    .unwrap()
    .with_basis_evaluator(Arc::new(PeriodicHarmonicEvaluator::new(m).unwrap()));

    let assignment = SaeAssignment::from_blocks_with_mode_and_manifolds(
        Array2::<f64>::zeros((n, 1)),
        vec![coords0_data],
        vec![LatentManifold::Circle { period: 1.0 }],
        AssignmentMode::softmax(0.5),
    )
    .unwrap();
    let mut term = SaeManifoldTerm::new(vec![atom], assignment).unwrap();
    let mut rho = SaeManifoldRho::new(0.0, -6.0, vec![Array1::<f64>::zeros(1)]);

    let max_iter = 10usize;
    let learning_rate = 1.0;
    let ridge = 1.0e-6;
    let mut prev_total = f64::INFINITY;
    for _ in 0..max_iter {
        let loss = term
            .run_joint_fit_arrow_schur(z.view(), &mut rho, None, 1, learning_rate, ridge, ridge)
            .unwrap();
        let total = loss.total();
        if !total.is_finite() {
            break;
        }
        let denom = prev_total.abs().max(1.0e-12);
        let rel = (prev_total - total).abs() / denom;
        prev_total = total;
        if rel < 1.0e-6 {
            break;
        }
    }

    let fitted = term.fitted();
    assert_eq!(fitted.dim(), (n, p));
    let mut ssr = 0.0;
    for i in 0..n {
        let r = z[[i, 0]] - fitted[[i, 0]];
        ssr += r * r;
    }
    let r2 = 1.0 - ssr / sst.max(1.0e-12);
    assert!(
        r2 >= 0.95,
        "10-step in-sample R² = {r2:.4} (ssr={ssr:.6}, sst={sst:.6}) should be >= 0.95"
    );
}

#[test]
pub(crate) fn sae_registry_refuses_assignment_sparsity_penalties() {
    let n = 3usize;
    let k = 2usize;
    let logits = Array2::<f64>::zeros((n, k));
    let coords: Vec<Array2<f64>> = (0..k).map(|_| Array2::<f64>::zeros((n, 1))).collect();
    let manifolds = vec![LatentManifold::Circle { period: 1.0 }; k];
    let assignment = SaeAssignment::from_blocks_with_mode_and_manifolds(
        logits,
        coords,
        manifolds,
        AssignmentMode::softmax(0.7),
    )
    .expect("valid assignment");
    let atoms: Vec<SaeManifoldAtom> = (0..k)
        .map(|atom_idx| {
            SaeManifoldAtom::new_with_provided_function_gram(
                format!("periodic_{atom_idx}"),
                SaeAtomBasisKind::Periodic,
                1,
                Array2::<f64>::ones((n, 1)),
                Array3::<f64>::zeros((n, 1, 1)),
                Array2::<f64>::zeros((1, 1)),
                Array2::<f64>::eye(1),
            )
            .expect("valid atom")
        })
        .collect();
    let term = SaeManifoldTerm::new(atoms, assignment).expect("valid SAE term");

    let mut softmax_registry = AnalyticPenaltyRegistry::new();
    softmax_registry.push(AnalyticPenaltyKind::SoftmaxAssignmentSparsity(Arc::new(
        gam_terms::analytic_penalties::SoftmaxAssignmentSparsityPenalty::new(k, 0.7),
    )));
    let softmax_err = term
        .validate_analytic_penalty_registry(&softmax_registry)
        .expect_err("SAE registry must reject softmax assignment sparsity");
    assert!(softmax_err.contains("assignment sparsity"));

    let mut ordered_beta_bernoulli_registry = AnalyticPenaltyRegistry::new();
    ordered_beta_bernoulli_registry.push(AnalyticPenaltyKind::OrderedBetaBernoulli(Arc::new(
        gam_terms::analytic_penalties::OrderedBetaBernoulliPenalty::new(k, 1.2, 0.7, false),
    )));
    let ordered_beta_bernoulli_err = term
        .validate_analytic_penalty_registry(&ordered_beta_bernoulli_registry)
        .expect_err("SAE registry must reject ordered Beta--Bernoulli assignment sparsity");
    assert!(ordered_beta_bernoulli_err.contains("assignment sparsity"));
}

/// Regression test for issue #174: K>=2 periodic atoms with zero-init
/// decoder used to collapse to A≈0 because the assignment prior was the
/// only term with non-zero gradient at iter 0. The pyffi entry point now
/// seeds decoder coefficients via a joint LSQ projection of Z onto
/// [a_init · Phi_k]. This test exercises that exact seeding strategy
/// in pure Rust and verifies the joint Newton fit reaches positive R²
/// on a clean K=2 periodic torus signal, mirroring the failing
/// reproducer in #174.
#[test]
pub(crate) fn ordered_beta_bernoulli_k2_periodic_torus_recovers_signal_with_lsq_init() {
    use faer::Side as FaerSide;
    use gam_linalg::faer_ndarray::{FaerCholesky, fast_ata, fast_atb};

    let n = 200usize;
    let p = 8usize;
    let k = 2usize;
    let m = 5usize; // 1 (constant) + 2 harmonics * 2 (sin/cos) = 5

    // Build a synthetic K=2 torus signal Z = [cos th1, sin th1, cos th2, sin th2] @ mix
    // with two latent angles. Deterministic seed via index arithmetic.
    let mut theta = Array2::<f64>::zeros((n, 2));
    for i in 0..n {
        theta[[i, 0]] = ((i as f64) * 0.07) % 1.0;
        theta[[i, 1]] = ((i as f64) * 0.13 + 0.31) % 1.0;
    }
    let mut raw = Array2::<f64>::zeros((n, 4));
    for i in 0..n {
        let a1 = 2.0 * std::f64::consts::PI * theta[[i, 0]];
        let a2 = 2.0 * std::f64::consts::PI * theta[[i, 1]];
        raw[[i, 0]] = a1.cos();
        raw[[i, 1]] = a1.sin();
        raw[[i, 2]] = a2.cos();
        raw[[i, 3]] = a2.sin();
    }
    // Deterministic 4x8 mixing matrix.
    let mix = Array2::<f64>::from_shape_fn((4, p), |(i, j)| {
        ((i as f64 + 1.0) * 0.37 + (j as f64) * 0.21).sin()
    });
    let mut z = Array2::<f64>::zeros((n, p));
    for i in 0..n {
        for j in 0..p {
            let mut acc = 0.0;
            for r in 0..4 {
                acc += raw[[i, r]] * mix[[r, j]];
            }
            z[[i, j]] = acc;
        }
    }
    // Centre Z so R² is well-defined relative to mean.
    let mut col_mean = Array1::<f64>::zeros(p);
    for j in 0..p {
        let mut acc = 0.0;
        for i in 0..n {
            acc += z[[i, j]];
        }
        col_mean[j] = acc / n as f64;
    }
    for i in 0..n {
        for j in 0..p {
            z[[i, j]] -= col_mean[j];
        }
    }

    // Atom coordinates: use the (shifted) true angles so the periodic
    // basis aligns with the signal — the test isolates the decoder-init
    // collapse, not coordinate recovery.
    let mut coords_k = vec![Array2::<f64>::zeros((n, 1)); k];
    for i in 0..n {
        coords_k[0][[i, 0]] = (theta[[i, 0]] + 0.05).rem_euclid(1.0);
        coords_k[1][[i, 0]] = (theta[[i, 1]] + 0.07).rem_euclid(1.0);
    }
    // Periodic basis (constant + 2 harmonics → M=5) for each atom.
    let evaluator = PeriodicHarmonicEvaluator::new(m).unwrap();
    let mut phi_k = Vec::with_capacity(k);
    let mut jet_k = Vec::with_capacity(k);
    for atom_idx in 0..k {
        let (phi, jet) = evaluator.evaluate(coords_k[atom_idx].view()).unwrap();
        phi_k.push(phi);
        jet_k.push(jet);
    }

    // LSQ seed: joint design X = [0.5 * Phi_1 | 0.5 * Phi_2] (ordered Beta--Bernoulli
    // logit 0 gives sigmoid(0/tau) = 0.5 for both atoms), solve normal
    // equations with a small ridge.
    let m_total = k * m;
    let mut x = Array2::<f64>::zeros((n, m_total));
    for atom_idx in 0..k {
        for i in 0..n {
            for col in 0..m {
                x[[i, atom_idx * m + col]] = 0.5 * phi_k[atom_idx][[i, col]];
            }
        }
    }
    let mut xtx = fast_ata(&x);
    let mut trace = 0.0_f64;
    for i in 0..m_total {
        trace += xtx[[i, i]];
    }
    let jitter = (trace / m_total as f64).max(1.0) * 1.0e-8;
    for i in 0..m_total {
        xtx[[i, i]] += jitter;
    }
    let xtz = fast_atb(&x, &z);
    let b_joint = xtx
        .cholesky(FaerSide::Lower)
        .expect("LSQ Cholesky")
        .solve_mat(&xtz);

    let mut atoms = Vec::with_capacity(k);
    for atom_idx in 0..k {
        let mut b = Array2::<f64>::zeros((m, p));
        for col in 0..m {
            for j in 0..p {
                b[[col, j]] = b_joint[[atom_idx * m + col, j]];
            }
        }
        let atom = SaeManifoldAtom::new_with_provided_function_gram(
            format!("torus_atom_{atom_idx}"),
            SaeAtomBasisKind::Periodic,
            1,
            phi_k[atom_idx].clone(),
            jet_k[atom_idx].clone(),
            b,
            Array2::<f64>::eye(m),
        )
        .unwrap()
        .with_basis_evaluator(Arc::new(PeriodicHarmonicEvaluator::new(m).unwrap()));
        atoms.push(atom);
    }
    let assignment = SaeAssignment::from_blocks_with_mode_and_manifolds(
        Array2::<f64>::zeros((n, k)),
        coords_k,
        vec![LatentManifold::Circle { period: 1.0 }; k],
        AssignmentMode::ordered_beta_bernoulli(0.7, 1.0, false),
    )
    .unwrap();
    let mut term = SaeManifoldTerm::new(atoms, assignment).unwrap();
    // `lambda_sparse` is the ordered Beta--Bernoulli assignment-sparsity prior weight (now wired
    // through `assignment_prior_grad_hdiag`'s ordered Beta--Bernoulli branch, #853). The
    // Beta-Bernoulli BCE energy toward the self-referential empirical active
    // fraction has its global minimum at the all-off gate, so at the old
    // full weight (`log_lambda_sparse = 0 → λ = 1`) it overwhelmed the
    // truth-seeded data fit and collapsed the assignment off both atoms. A
    // moderate prior weight keeps the sparsity pressure honest while letting
    // the LSQ-seeded reconstruction hold both real atoms active — the
    // realistic operating point this recovery test pins.
    let mut rho = SaeManifoldRho::new((0.02_f64).ln(), -6.0, vec![Array1::<f64>::zeros(1); k]);

    let mut prev_total = f64::INFINITY;
    for _ in 0..30 {
        let loss = term
            .run_joint_fit_arrow_schur(z.view(), &mut rho, None, 1, 1.0, 1.0e-6, 1.0e-6)
            .unwrap();
        let total = loss.total();
        if !total.is_finite() {
            break;
        }
        let denom = prev_total.abs().max(1.0e-12);
        let rel = (prev_total - total).abs() / denom;
        prev_total = total;
        if rel < 1.0e-6 {
            break;
        }
    }

    let fitted = term.fitted();
    let mut ssr = 0.0;
    let mut sst = 0.0;
    for i in 0..n {
        for j in 0..p {
            let r = z[[i, j]] - fitted[[i, j]];
            ssr += r * r;
            sst += z[[i, j]] * z[[i, j]];
        }
    }
    let r2 = 1.0 - ssr / sst.max(1.0e-12);
    assert!(
        r2 > 0.5,
        "K=2 periodic torus ordered Beta--Bernoulli R² = {r2:.4} (ssr={ssr:.4}, sst={sst:.4}) should be > 0.5 with LSQ-seeded decoder"
    );
    // Also confirm at least one atom remains active (assignment did not
    // collapse to ~0) — the active mass averaged over rows must exceed
    // a non-trivial threshold.
    let assignments = term.assignment.assignments();
    let mean_active: f64 = assignments.iter().copied().sum::<f64>() / (n as f64);
    assert!(
        mean_active > 0.2,
        "mean active mass across rows = {mean_active:.4} should exceed 0.2; assignment did not collapse"
    );
}

/// Regression test for issue #174 + #177 combined: softmax assignment
/// with K=2 periodic atoms should not crash and should reduce loss.
#[test]
pub(crate) fn softmax_k2_periodic_completes_joint_fit_step() {
    let n = 64usize;
    let p = 4usize;
    let k = 2usize;
    let m = 3usize;

    let mut z = Array2::<f64>::zeros((n, p));
    for i in 0..n {
        let a = 2.0 * std::f64::consts::PI * (i as f64) / (n as f64);
        z[[i, 0]] = a.sin();
        z[[i, 1]] = a.cos();
        z[[i, 2]] = (2.0 * a).sin();
        z[[i, 3]] = (2.0 * a).cos();
    }

    let evaluator = PeriodicHarmonicEvaluator::new(m).unwrap();
    let mut coords_k = vec![Array2::<f64>::zeros((n, 1)); k];
    for i in 0..n {
        coords_k[0][[i, 0]] = (i as f64) / (n as f64);
        coords_k[1][[i, 0]] = ((i as f64) * 2.0 / (n as f64)).rem_euclid(1.0);
    }
    let mut atoms = Vec::new();
    for atom_idx in 0..k {
        let (phi, jet) = evaluator.evaluate(coords_k[atom_idx].view()).unwrap();
        // Non-trivial decoder init (simulate LSQ seeding) so the data-fit
        // signal is non-zero at iter 0.
        let b = Array2::<f64>::from_shape_fn((m, p), |(i, j)| {
            0.1 * ((i as f64 + 1.0) * (j as f64 + 1.0)).sin()
        });
        let atom = SaeManifoldAtom::new_with_provided_function_gram(
            format!("a_{atom_idx}"),
            SaeAtomBasisKind::Periodic,
            1,
            phi,
            jet,
            b,
            Array2::<f64>::eye(m),
        )
        .unwrap()
        .with_basis_evaluator(Arc::new(PeriodicHarmonicEvaluator::new(m).unwrap()));
        atoms.push(atom);
    }
    let assignment = SaeAssignment::from_blocks_with_mode_and_manifolds(
        Array2::<f64>::zeros((n, k)),
        coords_k,
        vec![LatentManifold::Circle { period: 1.0 }; k],
        AssignmentMode::softmax(0.7),
    )
    .unwrap();
    let mut term = SaeManifoldTerm::new(atoms, assignment).unwrap();
    let mut rho = SaeManifoldRho::new(0.0, -6.0, vec![Array1::<f64>::zeros(1); k]);

    // First step must succeed (previously bailed with hessian-diag error).
    let loss0 = term
        .run_joint_fit_arrow_schur(z.view(), &mut rho, None, 1, 1.0, 1.0e-6, 1.0e-6)
        .expect("softmax K=2 must complete first joint-fit step");
    assert!(loss0.total().is_finite());
    let loss1 = term
        .run_joint_fit_arrow_schur(z.view(), &mut rho, None, 1, 1.0, 1.0e-6, 1.0e-6)
        .expect("softmax K=2 must complete second joint-fit step");
    assert!(loss1.total().is_finite());
}

/// End-to-end Isometry wiring oracle.
///
/// Build a SAE atom around an evaluator whose `second_jet` is now
/// implemented (periodic / sphere / torus), construct an
/// [`IsometryPenalty`] with matching `latent_dim` and `p_out`, refresh
/// the caches via [`refresh_isometry_caches_from_atom`], and check that
///
///   * `IsometryPenalty.value(target, rho)` is strictly positive (the
///     decoder we feed in is not orthonormal so the pullback metric is
///     not the identity, and the Euclidean reference picks up the gap).
///   * `IsometryPenalty.grad_target(target, rho)` is non-zero on at
///     least one latent-coordinate component.
///   * The analytic gradient matches a finite-difference oracle of
///     `value()` w.r.t. `target` (a single coord), where each FD probe
///     drives a fresh cache refresh — this is exactly the chain of
///     calls the SAE outer loop will make.
///
/// The FD oracle re-uses the existing [`refresh_isometry_caches_from_atom`]
/// helper for both the analytic side and the FD side, so any layout
/// mismatch between `J`/`H` would show up as a tolerance failure rather
/// than a silently zero gradient.
pub(crate) fn assert_isometry_wiring_matches_fd(
    evaluator: Arc<dyn SaeBasisSecondJet>,
    coords: Array2<f64>,
) {
    let n_obs = coords.nrows();
    let latent_dim = coords.ncols();
    let (phi, jet) = evaluator.evaluate(coords.view()).unwrap();
    let m = phi.ncols();
    let p: usize = 3;
    // A deterministic non-orthonormal decoder: deterministic LCG-ish
    // floats keep the test reproducible without needing rand.
    let mut decoder = Array2::<f64>::zeros((m, p));
    for i in 0..m {
        for j in 0..p {
            let x = (i as f64) * 0.371 + (j as f64) * 0.193 + 0.5;
            decoder[[i, j]] = (x.sin() * 0.9) + 0.1 * ((i + j) as f64).cos();
        }
    }
    let smooth = Array2::<f64>::eye(m);
    let atom = SaeManifoldAtom::new_with_provided_function_gram(
        "iso_wire_test",
        SaeAtomBasisKind::Periodic,
        latent_dim,
        phi.clone(),
        jet.clone(),
        decoder.clone(),
        smooth,
    )
    .unwrap()
    .with_basis_second_jet(evaluator);

    let target_slice = PsiSlice::full(n_obs * latent_dim, Some(latent_dim));
    let penalty = IsometryPenalty::new_euclidean(target_slice, p);
    let rho = Array1::<f64>::zeros(1);

    // Without a refresh, the safe default is zero and the gradient is
    // all zeros. Confirm the precondition so the post-refresh contrast
    // is meaningful.
    let target_flat: Array1<f64> = coords.iter().copied().collect();
    let v0 = penalty.value(target_flat.view(), rho.view());
    assert_eq!(v0, IsometryPenalty::DEFAULT_VALUE_ON_MISSING_CACHE);
    let g0 = penalty.grad_target(target_flat.view(), rho.view());
    assert!(
        g0.iter().all(|x| *x == 0.0),
        "grad_target without cache must be all zeros, got {g0:?}"
    );

    // Refresh and re-evaluate.
    let installed_second =
        refresh_isometry_caches_from_atom(&penalty, &atom, coords.view()).unwrap();
    assert!(
        installed_second,
        "evaluator must implement second_jet for this oracle to run"
    );

    let value = penalty.value(target_flat.view(), rho.view());
    assert!(
        value > 1.0e-6,
        "expected non-trivial isometry loss after cache refresh, got {value}"
    );
    let grad = penalty.grad_target(target_flat.view(), rho.view());
    assert_eq!(grad.len(), target_flat.len());
    let max_abs = grad.iter().fold(0.0_f64, |acc, x| acc.max(x.abs()));
    assert!(
        max_abs > 1.0e-6,
        "expected non-zero isometry gradient on at least one component, max |grad|={max_abs}"
    );

    // FD check: bump one coord, refresh, compare value(t±h e_j) against
    // analytic grad[j]. Pick coord (row 0, axis 0).
    let h_fd = 1.0e-5;
    let probe_idx = 0usize; // (row=0, axis=0) flattens to 0.
    let mut coords_plus = coords.clone();
    coords_plus[[0, 0]] += h_fd;
    let mut coords_minus = coords.clone();
    coords_minus[[0, 0]] -= h_fd;

    refresh_isometry_caches_from_atom(&penalty, &atom, coords_plus.view()).unwrap();
    let target_plus: Array1<f64> = coords_plus.iter().copied().collect();
    let v_plus = penalty.value(target_plus.view(), rho.view());

    refresh_isometry_caches_from_atom(&penalty, &atom, coords_minus.view()).unwrap();
    let target_minus: Array1<f64> = coords_minus.iter().copied().collect();
    let v_minus = penalty.value(target_minus.view(), rho.view());

    // Reinstall the base caches before reading grad at the base point.
    refresh_isometry_caches_from_atom(&penalty, &atom, coords.view()).unwrap();
    let grad_base = penalty.grad_target(target_flat.view(), rho.view());

    let fd = (v_plus - v_minus) / (2.0 * h_fd);
    let analytic = grad_base[probe_idx];
    // Both `value` and `grad_target` use the cached `J` (and `grad_target`
    // also the cached `H`). With finite differencing the cache itself,
    // the analytic-vs-FD agreement bounds the entire pipeline (J build,
    // H build, accessor read, pullback metric, gradient assembly) to
    // O(h²) error. Tolerance 1e-3 leaves headroom for the per-evaluator
    // characteristic magnitude.
    assert!(
        (analytic - fd).abs() <= 1.0e-3 + 1.0e-4 * analytic.abs().max(fd.abs()),
        "isometry grad/FD mismatch at coord 0: analytic={analytic:.6e}, fd={fd:.6e}"
    );
}

#[test]
pub(crate) fn isometry_wiring_periodic_matches_fd() {
    assert_isometry_wiring_matches_fd(
        Arc::new(PeriodicHarmonicEvaluator::new(5).unwrap()),
        array![[0.12], [0.37], [0.58], [0.81]],
    );
}

#[test]
pub(crate) fn isometry_wiring_sphere_matches_fd() {
    assert_isometry_wiring_matches_fd(
        Arc::new(AmbientSphereHarmonicEvaluator::new(2).unwrap()),
        array![
            [0.0, 0.0, 1.0],
            [0.6, -0.8, 0.0],
            [0.36, 0.48, 0.8]
        ],
    );
}

#[test]
pub(crate) fn isometry_wiring_torus_matches_fd() {
    assert_isometry_wiring_matches_fd(
        Arc::new(TorusHarmonicEvaluator::new(2, 2).unwrap()),
        array![[0.13, 0.42], [0.66, 0.19], [0.88, 0.55]],
    );
}

// [#780 line-count gate] The exact isometry-penalty HVP / PSD-majorizer
// cluster (`deterministic_decoder`, `build_isometry_atom_for_evaluator`,
// `assert_exact_isometry_hvp_*`, `assert_isometry_psd_majorizer_live_*`, the
// `isometry_exact_hvp_*` / `isometry_psd_majorizer_*` tests, and the
// `refresh_isometry_caches_pairs_each_penalty_to_its_own_atom` regression) was
// split into the sibling `tests_isometry_exact_hvp_majorizer_457.rs` module
// (declared in `mod.rs`) to keep this tracked file under the 10k limit. The
// cluster is self-contained: its helpers are referenced only within it.

/// Build a minimal single-atom periodic SAE outer objective for the
/// warm-start contract tests (gam#577 / gam#579).
pub(crate) fn warmstart_test_objective() -> SaeManifoldOuterObjective {
    // `PeriodicHarmonicEvaluator::new(3)` produces the SAME 3-column Fourier
    // basis `[1, sin(2πt), cos(2πt)]` and first jet as `periodic_basis`, plus
    // the analytic second jet that `logdet_theta_adjoint` (the softmax
    // assignment adjoint) needs. Installing it lets the full `eval` gradient
    // lane run instead of erroring on a missing second-jet evaluator.
    let evaluator = Arc::new(PeriodicHarmonicEvaluator::new(3).unwrap());
    let coords = array![[0.10], [0.35], [0.62], [0.88]];
    let (phi, jet) = evaluator.evaluate(coords.view()).unwrap();
    let atom = SaeManifoldAtom::new_with_provided_function_gram(
        "periodic",
        SaeAtomBasisKind::Periodic,
        1,
        phi,
        jet,
        // Decoder mapping the 3 basis fns to a single output channel.
        array![[0.30], [-0.20], [0.15]],
        // Mild ridge-like smoothness penalty so the inner solve is PD.
        Array2::<f64>::eye(3),
    )
    .unwrap()
    .with_basis_evaluator(evaluator.clone())
    .with_basis_second_jet(evaluator);
    let assignment = SaeAssignment::from_blocks_with_mode(
        // Nonzero assignment mass so H_tt carries genuine data curvature.
        array![[0.9_f64], [0.8], [0.7], [0.6]],
        vec![coords],
        AssignmentMode::softmax(0.7),
    )
    .unwrap();
    let term = SaeManifoldTerm::new(vec![atom], assignment).unwrap();
    let target = array![[0.20_f64], [-0.10], [0.30], [0.05]];
    let rho = SaeManifoldRho::new(0.0, 0.0, vec![Array1::<f64>::zeros(1)]);
    SaeManifoldOuterObjective::new(term, target, None, rho, 8, 1.0, 1.0e-6, 1.0e-6)
}

/// As [`warmstart_test_objective`], but the atom carries a full basis evaluator
/// AND second-jet evaluator (`PeriodicHarmonicEvaluator`), so the analytic outer
/// ρ-gradient lane (`eval` → `logdet_theta_adjoint`, which needs second jets for
/// the softmax assignment adjoint) can run. Required by the #1206 gradient-lane
/// contract test, which exercises the full `(cost, ∇f)` path.
pub(crate) fn warmstart_test_objective_with_evaluator() -> SaeManifoldOuterObjective {
    // `PeriodicHarmonicEvaluator::new(3)` produces the SAME 3-column Fourier
    // basis `[1, sin(2πt), cos(2πt)]` (1 harmonic) and matching first jet that
    // `periodic_basis` builds, so phi/jet are consistent with the decoder dims.
    let evaluator = Arc::new(PeriodicHarmonicEvaluator::new(3).unwrap());
    let coords = array![[0.10_f64], [0.35], [0.62], [0.88]];
    let (phi, jet) = evaluator.evaluate(coords.view()).unwrap();
    let atom = SaeManifoldAtom::new_with_provided_function_gram(
        "periodic",
        SaeAtomBasisKind::Periodic,
        1,
        phi,
        jet,
        array![[0.30_f64], [-0.20], [0.15]],
        Array2::<f64>::eye(3),
    )
    .unwrap()
    .with_basis_evaluator(evaluator.clone())
    .with_basis_second_jet(evaluator);
    let assignment = SaeAssignment::from_blocks_with_mode(
        array![[0.9_f64], [0.8], [0.7], [0.6]],
        vec![coords],
        AssignmentMode::softmax(0.7),
    )
    .unwrap();
    let term = SaeManifoldTerm::new(vec![atom], assignment).unwrap();
    let target = array![[0.20_f64], [-0.10], [0.30], [0.05]];
    let rho = SaeManifoldRho::new(0.0, 0.0, vec![Array1::<f64>::zeros(1)]);
    SaeManifoldOuterObjective::new(term, target, None, rho, 8, 1.0, 1.0e-6, 1.0e-6)
}

pub(crate) fn near_singular_outer_gradient_cache() -> ArrowFactorCache {
    ArrowFactorCache {
        htt_factors: ArrowFactorSlab::from_blocks(vec![array![[1.0_f64, 0.0], [0.0, 1.0e-7]]]),
        htt_factors_undamped: ArrowUndampedFactors::SameAsDamped,
        schur_factor: Some(array![[1.0_f64]]),
        schur_factor_is_undamped: true,
        beta_schur_conditioning: None,
        joint_hessian_log_det: None,
        solver_mode: ArrowSolverMode::Direct,
        ridge_t: 0.0,
        ridge_beta: 0.0,
        htbeta: ArrowHtbetaCache::Disabled { estimated_bytes: 0 },
        d: 2,
        row_dims: Arc::from(vec![2usize].into_boxed_slice()),
        row_offsets: Arc::from(vec![0usize, 2usize].into_boxed_slice()),
        k: 1,
        manifold_mode_fingerprint: 0,
        row_hessian_fingerprint: 0,
        pcg_diagnostics: ArrowPcgDiagnostics::default(),
        gauge_deflated_directions: 0,
        deflated_row_directions: std::sync::Arc::from(Vec::new()),
        deflation_row_spectra: std::sync::Arc::from(Vec::new()),
        beta_gauge_quotient: None,
    }
}

pub(crate) fn diagonal_latent_cache(diagonal: &[f64]) -> ArrowFactorCache {
    let dim = diagonal.len();
    let mut factor = Array2::<f64>::zeros((dim, dim));
    for i in 0..dim {
        factor[[i, i]] = diagonal[i].sqrt();
    }
    ArrowFactorCache {
        htt_factors: ArrowFactorSlab::from_blocks(vec![factor]),
        htt_factors_undamped: ArrowUndampedFactors::SameAsDamped,
        schur_factor: None,
        schur_factor_is_undamped: true,
        beta_schur_conditioning: None,
        joint_hessian_log_det: None,
        solver_mode: ArrowSolverMode::Direct,
        ridge_t: 0.0,
        ridge_beta: 0.0,
        htbeta: ArrowHtbetaCache::Disabled { estimated_bytes: 0 },
        d: dim,
        row_dims: Arc::from(vec![dim].into_boxed_slice()),
        row_offsets: Arc::from(vec![0usize, dim].into_boxed_slice()),
        k: 0,
        manifold_mode_fingerprint: 0,
        row_hessian_fingerprint: 0,
        pcg_diagnostics: ArrowPcgDiagnostics::default(),
        gauge_deflated_directions: 0,
        deflated_row_directions: std::sync::Arc::from(Vec::new()),
        deflation_row_spectra: std::sync::Arc::from(Vec::new()),
        beta_gauge_quotient: None,
    }
}

#[test]
pub(crate) fn outer_gradient_solver_rejects_near_singular_cache_without_matching_gauge() {
    let cache = near_singular_outer_gradient_cache();
    let obj = warmstart_test_objective();

    // The raw conditioning gate is what names the ill-conditioned joint Hessian
    // and reports the pivot ratio + floor. Pin that message HERE, at its source
    // (`outer_gradient_conditioning_error`), so the diagnostic stays covered even
    // though the solver below now re-classifies the gauge-degenerate case.
    let conditioning_err = match SaeManifoldTerm::outer_gradient_conditioning_error(&cache) {
        Err(err) => err.to_string(),
        Ok(()) => panic!("near-singular cache must trip the pivot-ratio conditioning gate"),
    };
    assert!(
        conditioning_err.contains("joint Hessian numerically singular"),
        "conditioning gate must name the ill-conditioned joint Hessian; got: {conditioning_err}"
    );
    assert!(
        conditioning_err.contains("min/max pivot ratio") && conditioning_err.contains("floor"),
        "conditioning gate must report the pivot ratio and floor; got: {conditioning_err}"
    );

    // #1436 (commit 21c49d14b): when the conditioning gate fires but NO chart
    // gauge / decoder-β-null / decoder-channel-null candidate can be recovered to
    // deflate the flat subspace, the flatness is genuinely OUTSIDE the gauge orbit
    // — a distinct, more specific diagnosis the solver surfaces as
    // `OuterGradientError::NonIdentifiable` (rather than echoing the raw
    // pivot-ratio `IllConditioned` trip). Both classes are FD-eligible, so the
    // recovery behaviour is unchanged; only the diagnostic is sharper. This is the
    // exact "without a matching gauge" path the test name describes.
    let err = match obj
        .term
        .outer_gradient_arrow_solver(&cache, &obj.current_rho.lambda_smooth_vec().unwrap())
    {
        Err(err) => err,
        Ok(..) => panic!("near-singular criterion factor without a matching gauge must reject"),
    };
    assert!(
        matches!(err, OuterGradientError::NonIdentifiable { .. }),
        "no-deflatable-direction rejection must be the NonIdentifiable diagnosis; got: {err}"
    );
    let err = err.to_string();
    assert!(
        err.contains("no deflatable gauge/decoder-null direction"),
        "guard error must name the absent deflation candidate; got: {err}"
    );
}

/// #1051: a euclidean-patch atom whose decoder design is RANK-DEFICIENT
/// (a straight line in a `p = 2` ambient: the decoder column space is rank
/// 1, so one output-channel direction is unidentified by the data) leaves a
/// genuine near-null direction of the joint Hessian in the β (decoder)
/// block. That direction is OUTSIDE the closed-form chart gauge orbit
/// (`dense_step_gauge_vectors` only spans per-latent-axis reparametrisation,
/// never per-output-channel decoder freedom), so before the fix
/// `outer_gradient_arrow_solver` could not deflate it and rejected the
/// trial ρ with "analytic outer gradient undefined" — the singular-pivot
/// continuation stall that made every euclidean/multi-atom atlas tile
/// TIMEOUT. With the β-basis admitted as a deflation candidate the flat
/// direction is Faddeev-Popov-deflated and the solve succeeds, regularising
/// the near-null β response to the Hessian scale (bounded, not 1e13).
pub(crate) fn rank_deficient_euclidean_outer_gradient_objective() -> SaeManifoldOuterObjective {
    // Linear euclidean basis Φ(t) = [1, t] (m = 2) over a 1-D latent.
    let coords = array![[-0.7_f64], [-0.2], [0.3], [0.8]];
    let n = coords.nrows();
    let mut phi = Array2::<f64>::zeros((n, 2));
    let mut jet = Array3::<f64>::zeros((n, 2, 1));
    for row in 0..n {
        phi[[row, 0]] = 1.0;
        phi[[row, 1]] = coords[[row, 0]];
        jet[[row, 1, 0]] = 1.0; // d/dt of the linear column.
    }
    // p = 2 ambient, but the decoder maps only into output channel 0 (its
    // second column is identically zero), so the reconstruction `Φ·B` lives on
    // the 1-D subspace `{x : x₁ = 0}` of R² and output channel 1 is genuinely
    // unidentified. The decoder's right-singular null vector is then exactly the
    // channel-1 axis `(0, 1)`, matching the near-null direction the joint-Hessian
    // cache below places on that axis (β indices 1 and 3). This is the rank-1
    // decoder column-span deficiency `decoder_channel_null_directions` must
    // recover (#1051/#1273).
    let decoder = array![[1.0_f64, 0.0], [0.5, 0.0]];
    let atom = SaeManifoldAtom::new_with_provided_function_gram(
        "euclidean_line",
        SaeAtomBasisKind::EuclideanPatch,
        1,
        phi,
        jet,
        decoder,
        Array2::<f64>::eye(2),
    )
    .unwrap();
    let assignment = SaeAssignment::from_blocks_with_mode(
        array![[0.9_f64], [0.8], [0.7], [0.6]],
        vec![coords],
        AssignmentMode::softmax(0.7),
    )
    .unwrap();
    let term = SaeManifoldTerm::new(vec![atom], assignment).unwrap();
    let target = array![[-1.0_f64, -2.0], [-0.3, -0.6], [0.4, 0.8], [1.1, 2.2]];
    let rho = SaeManifoldRho::new(0.0, 0.0, vec![Array1::<f64>::zeros(1)]);
    SaeManifoldOuterObjective::new(term, target, None, rho, 8, 1.0, 1.0e-6, 1.0e-6)
}

/// A joint Hessian cache whose β block carries one genuine near-null
/// direction along the SECOND output channel (`out_col = 1`) — the
/// rank-deficient decoder's unidentified direction — with the latent block
/// well-conditioned and `H_tβ = 0` so the singularity is purely in β. The
/// chart gauge orbit cannot reach this direction (#1051).
pub(crate) fn rank_deficient_beta_outer_gradient_cache() -> ArrowFactorCache {
    // The latent block must be dimensionally consistent with the paired
    // objective `rank_deficient_euclidean_outer_gradient_objective` so the
    // channel-null candidates (whose full length is the objective's
    // `n·q + β_dim`) survive the `dir.len() == full_len` guard in
    // `outer_gradient_arrow_solver`. That objective has n = 4 data rows and
    // `row_block_dim q = 1` (one latent axis, K = 1 softmax ⇒ no assignment
    // coord), so `delta_t_len` must be `n·q = 4`. A mismatched single-row cache
    // makes `full_len = 5` while the candidates have length 8, silently
    // dropping every channel-null direction and re-introducing the bug.
    let htt = ArrowFactorSlab::from_blocks(vec![
        array![[1.0_f64]],
        array![[1.0_f64]],
        array![[1.0_f64]],
        array![[1.0_f64]],
    ]);
    // β dim = m · p = 2 · 2 = 4, laid out (col, out_col) row-major like
    // `dense_step_gauge_vector_from_field`. Make output channel 1 (indices
    // 1 and 3) near-null: its lower-Cholesky pivot is 1e-7, so the
    // min/max pivot ratio falls below the 1e-12 floor and the conditioning
    // path engages. H_tβ = 0 (zero Dense blocks) decouples β from latent.
    let schur = array![
        [1.0_f64, 0.0, 0.0, 0.0],
        [0.0, 1.0e-7, 0.0, 0.0],
        [0.0, 0.0, 1.0, 0.0],
        [0.0, 0.0, 0.0, 1.0e-7],
    ];
    ArrowFactorCache {
        htt_factors: htt,
        htt_factors_undamped: ArrowUndampedFactors::SameAsDamped,
        schur_factor: Some(schur),
        schur_factor_is_undamped: true,
        beta_schur_conditioning: None,
        joint_hessian_log_det: None,
        solver_mode: ArrowSolverMode::Direct,
        ridge_t: 0.0,
        ridge_beta: 0.0,
        htbeta: ArrowHtbetaCache::Dense {
            blocks: Arc::from(
                vec![
                    Array2::<f64>::zeros((1, 4)),
                    Array2::<f64>::zeros((1, 4)),
                    Array2::<f64>::zeros((1, 4)),
                    Array2::<f64>::zeros((1, 4)),
                ]
                .into_boxed_slice(),
            ),
            estimated_bytes: 0,
        },
        d: 4,
        row_dims: Arc::from(vec![1usize, 1usize, 1usize, 1usize].into_boxed_slice()),
        row_offsets: Arc::from(vec![0usize, 1usize, 2usize, 3usize, 4usize].into_boxed_slice()),
        k: 4,
        manifold_mode_fingerprint: 0,
        row_hessian_fingerprint: 0,
        pcg_diagnostics: ArrowPcgDiagnostics::default(),
        gauge_deflated_directions: 0,
        deflated_row_directions: std::sync::Arc::from(Vec::new()),
        deflation_row_spectra: std::sync::Arc::from(Vec::new()),
        beta_gauge_quotient: None,
    }
}

#[test]
pub(crate) fn outer_gradient_solver_deflates_rank_deficient_decoder_beta_null() {
    let obj = rank_deficient_euclidean_outer_gradient_objective();
    let cache = rank_deficient_beta_outer_gradient_cache();
    // Sanity: the cache genuinely trips the conditioning floor (the bug's
    // precondition) — without it this test would not exercise the fix.
    assert!(
        SaeManifoldTerm::outer_gradient_conditioning_error(&cache).is_err(),
        "fixture must be sub-floor singular so the conditioning path engages"
    );
    // The fix: the β-block near-null direction is admitted as a deflation
    // candidate and Faddeev-Popov-deflated, so the solver SUCCEEDS instead
    // of rejecting with "analytic outer gradient undefined".
    let solver = obj
        .term
        .outer_gradient_arrow_solver(&cache, &obj.current_rho.lambda_smooth_vec().unwrap())
        .expect("rank-deficient decoder β-null must be deflated, not rejected (#1051/#1273)");
    // The deflated solve must REGULARISE the near-null β response: a plain
    // inverse divides by the 1e-7 pivot and explodes; the deflated solve is
    // bounded at the Hessian scale.
    let beta_null_rhs = array![0.0_f64, 0.0, 0.0, 1.0]; // output channel 1, col 1.
    let rhs_t = Array1::<f64>::zeros(cache.delta_t_len());
    let plain = cache
        .full_inverse_apply(rhs_t.view(), beta_null_rhs.view())
        .expect("plain solve")
        .1;
    let deflated = solver
        .solve(rhs_t.view(), beta_null_rhs.view())
        .expect("deflated solve")
        .beta;
    assert!(
        plain[3].abs() > 1.0e13,
        "plain near-null β solve must explode; got {}",
        plain[3]
    );
    assert!(
        deflated.iter().all(|v| v.is_finite()) && deflated[3].abs() < 10.0,
        "deflated near-null β solve must be bounded at the Hessian scale; got {deflated:?}"
    );
}

/// #1436 — the analytic derivative error taxonomy must keep internal-invariant
/// failures distinct from genuine conditioning/non-identifiability. Every class
/// propagates if the projected solve cannot produce a reliable derivative, but
/// the diagnostic must remain machine-distinguishable.
#[test]
pub(crate) fn outer_gradient_internal_invariant_is_typed_1436() {
    let ill_conditioned = OuterGradientError::IllConditioned {
        reason: "near-singular joint Hessian".to_string(),
    };
    let non_identifiable = OuterGradientError::NonIdentifiable {
        reason: "gauge-degenerate direction".to_string(),
    };
    let internal = OuterGradientError::InternalInvariant {
        reason: "shape mismatch".to_string(),
    };
    assert!(ill_conditioned.to_string().contains("ill-conditioned"));
    assert!(non_identifiable.to_string().contains("non-identifiable"));
    assert!(
        internal.to_string().contains("internal invariant"),
        "InternalInvariant Display must name the class; got: {}",
        internal
    );
}

/// #2653 — an exact implicit-gradient solve can be undefined at one otherwise
/// finite line-search rho while remaining well-defined at the incumbent. Keep
/// conditioning/non-identifiability rho-local so BFGS contracts the trial;
/// invariant violations still invalidate the whole optimization.
#[test]
pub(crate) fn outer_gradient_failure_preserves_rho_locality_2653() {
    for error in [
        OuterGradientError::IllConditioned {
            reason: "finite projected solve lost residual reduction".to_string(),
        },
        OuterGradientError::NonIdentifiable {
            reason: "gauge-deflated operator remains singular".to_string(),
        },
    ] {
        let error = EstimationError::from(error);
        assert!(
            matches!(error, EstimationError::TrialPointRefused { .. })
                && error.is_trial_point_infeasible(),
            "conditioning at one rho must reject only that trial: {error}"
        );
    }

    let invariant = EstimationError::from(OuterGradientError::InternalInvariant {
        reason: "gradient length differs from rho layout".to_string(),
    });
    assert!(
        matches!(invariant, EstimationError::RemlOptimizationFailed(_))
            && !invariant.is_trial_point_infeasible(),
        "an invariant violation must remain fatal: {invariant}"
    );
}

/// An empty β means that cache or typed reactive entry has no coefficient
/// state to install. The hook must preserve the objective-owned state and
/// report `NoSlot`, rather than interpreting zero length as a decoder mismatch.
#[test]
pub(crate) fn seed_inner_state_accepts_empty_beta_as_noslot() {
    let mut obj = warmstart_test_objective();
    let empty: Array1<f64> = Array1::zeros(0);
    let outcome = obj
        .seed_inner_state(&empty)
        .expect("empty-β seed must be accepted as a no-op, not rejected (gam#577/#579)");
    assert!(
        matches!(outcome, SeedOutcome::NoSlot),
        "empty-β seed must report NoSlot (proceed cold); got {outcome:?}"
    );
}

/// A populated β whose length matches the decoder dimension must be
/// INSTALLED and then GENUINELY REUSED by the next inner solve — this is
/// the exact-seed cache and typed reactive waypoint contract rely on. We verify
/// reuse behaviorally with a β produced by a converged evidence solve, then run
/// one eval with zero inner Newton iterations and confirm the published
/// `inner_beta_hint` is exactly that seed. An arbitrary off-optimum β can have no
/// defined frozen quasi-Laplace score and is not a valid ownership witness.
#[test]
pub(crate) fn seed_inner_state_installs_and_reuses_matching_beta() {
    let mut source = warmstart_test_objective();
    let source_rho = source.baseline_rho.clone();
    source
        .term
        .penalized_quasi_laplace_criterion_with_cache(
            source.target.view(),
            &source_rho,
            source.registry.as_ref(),
            source.inner_max_iter,
            source.learning_rate,
            source.ridge_ext_coord,
            source.ridge_beta,
        )
        .expect("source continuation state must have finite converged evidence");
    let seed = source.term.flatten_beta();

    let mut obj = warmstart_test_objective();
    let dim = obj.term.beta_dim();
    let pristine = obj.term.flatten_beta();
    assert_eq!(seed.len(), dim, "source β must match the target layout");
    assert!(
        (&seed - &pristine).iter().any(|d| d.abs() > 1e-6),
        "converged continuation β must differ from the pristine target β for the reuse check"
    );

    let outcome = obj
        .seed_inner_state(&seed)
        .expect("a length-matching β must install");
    assert!(
        matches!(outcome, SeedOutcome::Installed),
        "matching β must report Installed; got {outcome:?}"
    );

    // Freeze the inner solve at zero Newton iterations: β cannot move off
    // the warm-start, so the published hint must equal the seed exactly.
    obj.inner_max_iter = 0;
    let rho_flat = obj.baseline_rho.to_flat();
    let eval =
        OuterObjective::eval(&mut obj, &rho_flat).expect("eval at the warm-started β must succeed");
    let hint = eval
        .inner_beta_hint
        .expect("the SAE objective must publish inner_beta_hint for continuation reuse");
    assert_eq!(
        hint.len(),
        dim,
        "published hint must have decoder dimension"
    );
    for (i, (&h, &s)) in hint.iter().zip(seed.iter()).enumerate() {
        assert!(
            (h - s).abs() < 1e-12,
            "warm-started β must be reused verbatim by the inner solve at coord {i}: \
                 hint {h} != seed {s} (gam#577/#579)"
        );
    }
}

/// The seed contract is only relaxed for the EMPTY sentinel. A populated
/// β whose length disagrees with the decoder dimension is a genuine
/// layout bug and must still surface a typed error rather than being
/// silently dropped.
#[test]
pub(crate) fn seed_inner_state_rejects_wrong_length_populated_beta() {
    let mut obj = warmstart_test_objective();
    let dim = obj.term.beta_dim();
    let wrong: Array1<f64> = Array1::zeros(dim + 1);
    let err = obj
        .seed_inner_state(&wrong)
        .expect_err("a populated β of the wrong length must be rejected");
    match err {
        EstimationError::RemlOptimizationFailed(msg) => {
            assert!(
                msg.contains("decoder dim"),
                "error must name the decoder-dim mismatch; got: {msg}"
            );
        }
        other => panic!("expected RemlOptimizationFailed, got {other:?}"),
    }
}

pub(crate) fn gamma_fd_tiny_fixture() -> (SaeManifoldTerm, Array2<f64>, SaeManifoldRho) {
    let n = 10usize;
    let p = 3usize;
    let k_atoms = 2usize;
    let m = 3usize;
    let evaluator = Arc::new(PeriodicHarmonicEvaluator::new(m).unwrap());
    let mut logits = Array2::<f64>::zeros((n, k_atoms));
    let mut coords = vec![Array2::<f64>::zeros((n, 1)), Array2::<f64>::zeros((n, 1))];
    let weights = [
        [
            [0.10, -0.05, 0.03],
            [0.35, -0.20, 0.12],
            [-0.16, 0.18, 0.08],
        ],
        [
            [-0.08, 0.04, 0.06],
            [0.22, 0.10, -0.18],
            [0.11, -0.24, 0.15],
        ],
    ];
    let mut target = Array2::<f64>::zeros((n, p));
    for row in 0..n {
        let phase = (row as f64 + 0.35) / n as f64;
        coords[0][[row, 0]] = phase;
        coords[1][[row, 0]] = (phase + 0.21).fract();
        logits[[row, 0]] = if row % 2 == 0 { 0.8 } else { -0.6 };
        let assignments = softmax_row(logits.row(row), 0.9);
        for atom in 0..k_atoms {
            let theta = std::f64::consts::TAU * coords[atom][[row, 0]];
            let basis = [1.0, theta.sin(), theta.cos()];
            for out_col in 0..p {
                for basis_col in 0..m {
                    target[[row, out_col]] +=
                        assignments[atom] * basis[basis_col] * weights[atom][basis_col][out_col];
                }
            }
        }
    }
    let mut atoms = Vec::with_capacity(k_atoms);
    for atom in 0..k_atoms {
        let (phi, jet) = evaluator.evaluate(coords[atom].view()).unwrap();
        let decoder = Array2::from_shape_fn((m, p), |(basis_col, out_col)| {
            weights[atom][basis_col][out_col]
        });
        atoms.push(
            SaeManifoldAtom::new_with_provided_function_gram(
                format!("gamma_{atom}"),
                SaeAtomBasisKind::Periodic,
                1,
                phi,
                jet,
                decoder,
                Array2::<f64>::eye(m),
            )
            .unwrap()
            .with_basis_second_jet(evaluator.clone()),
        );
    }
    let assignment = SaeAssignment::from_blocks_with_mode_and_manifolds(
        logits,
        coords,
        vec![LatentManifold::Circle { period: 1.0 }; k_atoms],
        AssignmentMode::softmax(0.9),
    )
    .unwrap();
    let term = SaeManifoldTerm::new(atoms, assignment).unwrap();
    let rho = SaeManifoldRho::new(
        -6.0,
        -6.0,
        vec![Array1::from_vec(vec![-6.0]), Array1::from_vec(vec![-6.0])],
    );
    (term, target, rho)
}

// [#780 line-count gate] The #1557 arrow-Schur parallelism-invariance
// regression test (`arrow_schur_assembly_is_faer_parallelism_invariant_1557`)
// was split into the sibling `tests_parallelism_invariance_1557.rs` module
// (declared in `mod.rs`) to keep this tracked file under the 10k limit.
//
// The stationary-cache `∂log|H|/∂θ` adjoint and assignment-prior trace
// regressions were likewise split into the sibling
// `tests_logdet_adjoint_780.rs` module for the same gate; they still source the
// shared `gamma_fd_tiny_fixture` / `fixed_state_logdet_sample` helpers, which remain
// defined here.