gam-terms 0.3.152

use super::*;

use super::invariant_tie_break::resolve_sorted_profile_tie;

#[derive(Debug, Clone, Copy, PartialEq, Eq, Hash)]
pub(crate) struct ConstraintNullspaceCacheKey {
    pub(crate) centersrows: usize,
    pub(crate) centers_cols: usize,
    pub(crate) centers_hash: u64,
    pub(crate) order: ConstraintNullspaceOrderKey,
}

#[derive(Debug, Clone, Copy, PartialEq, Eq, Hash)]
pub(crate) enum ConstraintNullspaceOrderKey {
    Duchon(DuchonNullspaceOrder),
    ThinPlate,
}

#[derive(Default, Clone, Debug)]
pub(crate) struct ConstraintNullspaceCache {
    pub(crate) map: HashMap<ConstraintNullspaceCacheKey, Arc<Array2<f64>>>,
    pub(crate) order: Vec<ConstraintNullspaceCacheKey>,
}

pub(crate) const CONSTRAINT_NULLSPACE_CACHE_MAX_ENTRIES: usize = 32;

#[derive(Debug, Clone, Copy, PartialEq, Eq, Hash)]
pub(crate) struct OwnedDataCacheKey {
    pub(crate) rows: usize,
    pub(crate) cols: usize,
    pub(crate) ptr: usize,
    pub(crate) stride0: isize,
    pub(crate) stride1: isize,
}

#[derive(Debug)]
pub(crate) struct BasisCacheContext {
    pub(crate) constraint_nullspace: ConstraintNullspaceCache,
    pub(crate) owned_data: gam_runtime::resource::ByteLruCache<OwnedDataCacheKey, Arc<Array2<f64>>>,
}

impl BasisCacheContext {
    pub(crate) fn with_policy(policy: &gam_runtime::resource::ResourcePolicy) -> Self {
        Self {
            constraint_nullspace: ConstraintNullspaceCache::default(),
            owned_data: gam_runtime::resource::ByteLruCache::with_max_entries(
                policy.max_owned_data_cache_bytes,
                gam_runtime::resource::OWNED_DATA_CACHE_MAX_ENTRIES,
            ),
        }
    }
}

impl Default for BasisCacheContext {
    fn default() -> Self {
        Self::with_policy(&gam_runtime::resource::ResourcePolicy::default_library())
    }
}

/// Explicit per-run workspace for reusable basis-construction caches.
///
/// Pass one workspace through repeated basis builds to avoid global mutable state
/// and to keep caching scoped to a caller-controlled lifecycle.
///
/// Owned-data cache entries are byte-limited via the
/// [`gam_runtime::resource::ResourcePolicy`] provided at construction; use
/// [`BasisWorkspace::with_policy`] for large-scale workloads where a single
/// entry can be multiple gigabytes.
#[derive(Debug)]
pub struct BasisWorkspace {
    pub(crate) cache: BasisCacheContext,
    pub(crate) policy: gam_runtime::resource::ResourcePolicy,
}

impl BasisWorkspace {
    pub fn new() -> Self {
        Self::default()
    }

    pub fn with_policy(policy: gam_runtime::resource::ResourcePolicy) -> Self {
        Self {
            cache: BasisCacheContext::with_policy(&policy),
            policy,
        }
    }

    pub fn default_library() -> Self {
        Self::with_policy(gam_runtime::resource::ResourcePolicy::default_library())
    }

    /// Returns the resource policy this workspace was configured with.
    pub fn policy(&self) -> &gam_runtime::resource::ResourcePolicy {
        &self.policy
    }
}

impl Default for BasisWorkspace {
    fn default() -> Self {
        Self::default_library()
    }
}

pub(crate) fn hash_arrayview2(values: ArrayView2<'_, f64>) -> u64 {
    let mut hasher = DefaultHasher::new();
    values.nrows().hash(&mut hasher);
    values.ncols().hash(&mut hasher);
    for v in values {
        v.to_bits().hash(&mut hasher);
    }
    hasher.finish()
}

pub(crate) fn shared_owned_data_matrix(
    data: ArrayView2<'_, f64>,
    cache: &BasisCacheContext,
) -> Arc<Array2<f64>> {
    let key = OwnedDataCacheKey {
        rows: data.nrows(),
        cols: data.ncols(),
        ptr: data.as_ptr() as usize,
        stride0: data.strides()[0],
        stride1: data.strides()[1],
    };
    if let Some(hit) = cache.owned_data.get(&key) {
        return hit;
    }

    let owned = Arc::new(data.to_owned());
    if let Some(hit) = cache.owned_data.get(&key) {
        return hit;
    }

    cache.owned_data.insert(key, owned.clone());
    owned
}

/// Minimal cache-less intern: wraps an `ArrayView2` into an `Arc<Array2<f64>>`.
///
/// Used by derivative-operator builders that don't have a `BasisCacheContext`
/// in scope (e.g. `build_aniso_design_psi_derivatives_shared`). The goal is the
/// same as `shared_owned_data_matrix`: move the owned payload into an `Arc`
/// once so that downstream `StreamingRadialState` copies share it via
/// `Arc::clone` instead of materializing a fresh n×d `Array2<f64>` per axis.
#[inline]
pub(crate) fn shared_owned_data_matrix_from_view(data: ArrayView2<'_, f64>) -> Arc<Array2<f64>> {
    Arc::new(data.to_owned())
}

/// Minimal cache-less intern for knot centers; mirrors
/// `shared_owned_data_matrix_from_view`. Centers are typically k×d with k
/// much smaller than n, but the `Arc::clone` pattern still avoids a k×d
/// copy per axis when the same operator feeds multiple derivative paths.
#[inline]
pub(crate) fn shared_owned_centers_matrix_from_view(
    centers: ArrayView2<'_, f64>,
) -> Arc<Array2<f64>> {
    Arc::new(centers.to_owned())
}

/// Compute the kernel reparameterisation transform `Z = null(P_centers^T)`.
///
/// `Z` is a `(k, k − C(d+r, r))` orthonormal matrix whose columns span the
/// null space of the polynomial side-condition system.  Reparameterising the
/// radial kernel coefficients as `α = Z γ` enforces `P_centers^T α = 0` and
/// reduces the kernel column count from `k` to `k − C(d+r, r)`.
///
/// After this projection the polynomial block `P_data` is appended as separate
/// explicit unpenalized columns (see `build_duchon_basis_designwithworkspace`),
/// so the pre-identifiability total width is always `k` (equal to the center
/// count), regardless of the polynomial null-space dimension.
///
/// This is the step that absorbs the full `C(d+r, r)`-dimensional polynomial
/// null space.  The subsequent `spatial_parametric_constraint_block` step only
/// removes the intercept.
pub(crate) fn kernel_constraint_nullspace(
    centers: ArrayView2<'_, f64>,
    order: DuchonNullspaceOrder,
    cache: &mut BasisCacheContext,
) -> Result<Array2<f64>, BasisError> {
    let effective_order = duchon_effective_nullspace_order(centers, order);
    let centers_centered = mean_centered_centers(centers);
    let centers = centers_centered.view();
    let key = ConstraintNullspaceCacheKey {
        centersrows: centers.nrows(),
        centers_cols: centers.ncols(),
        centers_hash: hash_arrayview2(centers),
        order: ConstraintNullspaceOrderKey::Duchon(effective_order),
    };

    if let Some(hit) = cache.constraint_nullspace.map.get(&key) {
        return Ok((**hit).clone());
    }

    let z = Arc::new(duchon_constraint_nullspace_of_centered(
        centers,
        order,
        effective_order,
    )?);

    if let Some(hit) = cache.constraint_nullspace.map.get(&key) {
        return Ok((**hit).clone());
    }
    cache.constraint_nullspace.map.insert(key, z.clone());
    cache.constraint_nullspace.order.push(key);
    while cache.constraint_nullspace.map.len() > CONSTRAINT_NULLSPACE_CACHE_MAX_ENTRIES {
        if cache.constraint_nullspace.order.is_empty() {
            break;
        }
        let oldkey = cache.constraint_nullspace.order.remove(0);
        cache.constraint_nullspace.map.remove(&oldkey);
    }

    Ok((*z).clone())
}

/// Translation-invariant side-condition frame (#1375, mirroring the #1269 tp
/// fix). `Z = null(P(centers)ᵀ)` is mathematically invariant to subtracting a
/// per-axis constant from `centers` (the polynomial columns `{1, x, …}` and
/// `{1, x − x̄, …}` span the same space, so `P` has the same column space and
/// `P^T` the same null space), but the RRQR pivoting that materialises `Z`
/// drifts under a large coordinate mean — landing on a different orthonormal
/// basis of the SAME null space, which would desync the design `K·Z` from the
/// penalty `ZᵀK_CC Z` across a covariate translation. Subtract the center-cloud
/// per-axis mean so the factorisation is location-standardized; both a raw and
/// an already-centered caller then produce bit-identical `Z`. The mean is a
/// fixed property of the (frozen `UserProvided`) centers, replayed identically
/// at predict.
fn mean_centered_centers(centers: ArrayView2<'_, f64>) -> Array2<f64> {
    let k = centers.nrows();
    let d = centers.ncols();
    let center_mean: Vec<f64> = (0..d)
        .map(|c| centers.column(c).sum() / (k.max(1) as f64))
        .collect();
    let mut centers_centered = centers.to_owned();
    for c in 0..d {
        let mu = center_mean[c];
        centers_centered.column_mut(c).mapv_inplace(|v| v - mu);
    }
    centers_centered
}

/// Factor `Z = null(P(centers)ᵀ)` for centers that are ALREADY mean-centered,
/// wrapping a degradation context around the failure when the effective order
/// was auto-degraded below the requested one.
fn duchon_constraint_nullspace_of_centered(
    centers: ArrayView2<'_, f64>,
    order: DuchonNullspaceOrder,
    effective_order: DuchonNullspaceOrder,
) -> Result<Array2<f64>, BasisError> {
    let degraded = effective_order != order;
    let p_k = polynomial_block_from_order(centers, effective_order);
    kernel_constraint_nullspace_from_matrix(p_k.view()).map_err(|err| {
        if degraded {
            BasisError::InvalidInput(format!(
                "Duchon degraded from order={:?} to order={:?} due to insufficient centers ({} in dim={}); order={:?} construction then failed: {err}",
                order,
                effective_order,
                centers.nrows(),
                centers.ncols(),
                effective_order,
            ))
        } else {
            err
        }
    })
}

/// Cache-free canonical Duchon kernel-constraint null space: the SAME
/// degrade → mean-center → RRQR construction the cached design path uses.
/// Every consumer of a Duchon `Z` outside the workspace-cached design builder
/// (e.g. the FFI derivative jets, which must be the exact column-for-column
/// derivative of the forward design) must route through this one construction;
/// re-deriving `Z` without the centering lands on a different orthonormal
/// basis of the same null space and silently desyncs the jet's frame from the
/// design's.
pub fn duchon_kernel_constraint_nullspace(
    centers: ArrayView2<'_, f64>,
    order: DuchonNullspaceOrder,
) -> Result<Array2<f64>, BasisError> {
    let effective_order = duchon_effective_nullspace_order(centers, order);
    let centers_centered = mean_centered_centers(centers);
    duchon_constraint_nullspace_of_centered(centers_centered.view(), order, effective_order)
}

pub(crate) fn thin_plate_kernel_constraint_nullspace(
    centers: ArrayView2<'_, f64>,
    cache: &mut BasisCacheContext,
) -> Result<Array2<f64>, BasisError> {
    let key = ConstraintNullspaceCacheKey {
        centersrows: centers.nrows(),
        centers_cols: centers.ncols(),
        centers_hash: hash_arrayview2(centers),
        order: ConstraintNullspaceOrderKey::ThinPlate,
    };

    if let Some(hit) = cache.constraint_nullspace.map.get(&key) {
        return Ok((**hit).clone());
    }

    let p_k = thin_plate_polynomial_block(centers);
    if centers.nrows() < p_k.ncols() {
        crate::bail_invalid_basis!(
            "thin-plate spline requires at least {} centers to span the degree-{} polynomial null space in dimension {}; got {}",
            p_k.ncols(),
            thin_plate_polynomial_degree(centers.ncols()),
            centers.ncols(),
            centers.nrows()
        );
    }
    let (z, rank) =
        rrqr_nullspace_basis(&p_k, default_rrqr_rank_alpha()).map_err(BasisError::LinalgError)?;
    if rank != p_k.ncols() {
        crate::bail_invalid_basis!(
            "thin-plate spline polynomial block is rank deficient at the selected centers: expected rank {}, got {}; choose geometrically independent centers for dimension {}",
            p_k.ncols(),
            rank,
            centers.ncols()
        );
    }
    let z = Arc::new(z);

    if let Some(hit) = cache.constraint_nullspace.map.get(&key) {
        return Ok((**hit).clone());
    }
    cache.constraint_nullspace.map.insert(key, z.clone());
    cache.constraint_nullspace.order.push(key);
    while cache.constraint_nullspace.map.len() > CONSTRAINT_NULLSPACE_CACHE_MAX_ENTRIES {
        if cache.constraint_nullspace.order.is_empty() {
            break;
        }
        let oldkey = cache.constraint_nullspace.order.remove(0);
        cache.constraint_nullspace.map.remove(&oldkey);
    }

    Ok((*z).clone())
}

pub(crate) fn matern_identifiability_transform(
    centers: ArrayView2<'_, f64>,
    identifiability: &MaternIdentifiability,
) -> Result<Option<Array2<f64>>, BasisError> {
    let k = centers.nrows();
    match identifiability {
        MaternIdentifiability::None => Ok(None),
        MaternIdentifiability::CenterSumToZero => {
            let q = Array2::<f64>::ones((k, 1));
            Ok(Some(kernel_constraint_nullspace_from_matrix(q.view())?))
        }
        MaternIdentifiability::CenterLinearOrthogonal => {
            // Mirror the Duchon path: auto-degrade to Zero (constant-only) when
            // there aren't enough centers to affinely span [1, x_1, ..., x_d].
            // kernel_constraint_nullspace_from_matrix would otherwise hard-error
            // via rrqr_nullspace_basis when centers.nrows() < d + 1.
            let effective_order =
                duchon_effective_nullspace_order(centers, DuchonNullspaceOrder::Linear);
            let q = polynomial_block_from_order(centers, effective_order);
            Ok(Some(kernel_constraint_nullspace_from_matrix(q.view())?))
        }
        MaternIdentifiability::FrozenTransform { transform, .. } => {
            if transform.nrows() != k {
                crate::bail_dim_basis!(
                    "frozen Matérn identifiability transform mismatch: centers={k}, transform rows={}",
                    transform.nrows()
                );
            }
            Ok(Some(transform.clone()))
        }
    }
}

pub(crate) fn build_matern_operator_penalty_candidates(
    centers: ArrayView2<'_, f64>,
    length_scale: f64,
    nu: MaternNu,
    include_intercept: bool,
    z_opt: Option<&Array2<f64>>,
    aniso_log_scales: Option<&[f64]>,
) -> Result<Vec<PenaltyCandidate>, BasisError> {
    let ops = build_matern_collocation_operator_matrices(
        centers,
        None,
        length_scale,
        nu,
        include_intercept,
        z_opt.map(|z| z.view()),
        aniso_log_scales,
    )?;
    // Gate the operator dials on the Matérn-ν RKHS smoothness so a rough kernel
    // (e.g. ν=1/2) is not over-smoothed by a higher-order roughness penalty its
    // own RKHS norm does not control (#707).
    let matern_spec = DuchonOperatorPenaltySpec::matern_for_smoothness(nu, centers.ncols());
    operator_penalty_candidates_from_collocation(&ops.d0, &ops.d1, &ops.d2, &matern_spec)
}

/// True when every entry of `m` is finite.
fn matrix_all_finite(m: &Array2<f64>) -> bool {
    m.iter().all(|v| v.is_finite())
}

/// Discrete function Gram on Matérn's frozen center support.
///
/// The embedded primary contains `K_CC` in its kernel block. Evaluating the
/// represented raw basis at the same centers gives `[K_CC | 1]`; applying the
/// final kernel-identifiability chart and taking `B_CᵀB_C` therefore provides
/// an exact compact Gram for this finite-rank representation without touching
/// the training rows.
pub(crate) fn matern_center_function_gram(
    embedded_kernel: &Array2<f64>,
    include_intercept: bool,
    full_transform: Option<&Array2<f64>>,
) -> Result<Array2<f64>, BasisError> {
    if embedded_kernel.nrows() != embedded_kernel.ncols() {
        crate::bail_dim_basis!("Matérn embedded kernel penalty must be square");
    }
    let total = embedded_kernel.nrows();
    let k = total
        .checked_sub(usize::from(include_intercept))
        .ok_or_else(|| BasisError::InvalidInput("Matérn basis width underflow".to_string()))?;
    if k == 0 {
        crate::bail_invalid_basis!("Matérn function metric requires at least one center");
    }
    let mut center_design = Array2::<f64>::zeros((k, total));
    center_design
        .slice_mut(s![.., 0..k])
        .assign(&embedded_kernel.slice(s![0..k, 0..k]));
    if include_intercept {
        center_design.column_mut(k).fill(1.0);
    }
    let center_design = match full_transform {
        Some(transform) => fast_ab(&center_design, transform),
        None => center_design,
    };
    Ok(symmetrize_penalty(&fast_ata(&center_design)))
}

pub(crate) fn matern_double_penalty_candidates(
    primary: &Array2<f64>,
    function_gram: &Array2<f64>,
    include_intercept: bool,
) -> Result<Vec<PenaltyCandidate>, BasisError> {
    // gam#1379 — guard the Primary projected kernel Gram itself. It is `Zᵀ K Z`
    // with a finite Matérn kernel `K`, so it is finite in exact arithmetic; if a
    // degenerate trial geometry made it non-finite we cannot ship it as a
    // penalty (the range-block eigensolve would abort the fit). Surface a clear
    // basis error instead of an opaque downstream "non-finite range penalty".
    if !matrix_all_finite(primary) {
        crate::bail_invalid_basis!(
            "Matérn double-penalty primary kernel Gram is non-finite; the projected \
             kernel `Zᵀ K Z` could not be formed at this length scale (degenerate \
             geometry). Widen the data spread, change the length scale, or drop the term."
        );
    }
    if primary.dim() != function_gram.dim() || !matrix_all_finite(function_gram) {
        crate::bail_invalid_basis!(
            "Matérn center function Gram is non-finite or does not match the primary penalty"
        );
    }
    let mut candidates = vec![normalize_penalty_candidate(
        primary.clone(),
        PenaltySource::Primary,
    )?];
    // K_CC is strictly positive definite after center rank reduction. The ONLY
    // structural null direction is the explicitly appended intercept. Kernel
    // eigenvalues near a floating-point tolerance remain range directions; they
    // must be conditioned/reduced, never reclassified into a κ-dependent null
    // projector. This makes penalty topology structural and κ-invariant.
    if include_intercept {
        let p = primary.nrows();
        let mut intercept_frame = Array2::<f64>::zeros((p, 1));
        intercept_frame[[p - 1, 0]] = 1.0;
        let shrinkage = function_space_subspace_shrinkage(&intercept_frame, function_gram)?;
        candidates.push(normalize_penalty_candidate(
            shrinkage,
            PenaltySource::DoublePenaltyNullspace,
        )?);
    }
    Ok(candidates)
}

pub(crate) fn build_matern_double_penalty_candidates(
    spline: &MaternSplineBasis,
    full_transform: Option<&Array2<f64>>,
) -> Result<Vec<PenaltyCandidate>, BasisError> {
    let primary = project_penalty_matrix(&spline.penalty_kernel, full_transform);
    let include_intercept = spline.num_polynomial_basis == 1;
    let function_gram =
        matern_center_function_gram(&spline.penalty_kernel, include_intercept, full_transform)?;
    matern_double_penalty_candidates(&primary, &function_gram, include_intercept)
}

/// Creates a Matérn spline basis from data and centers.
///
/// The design is `[K | 1]` when `include_intercept=true` and `[K]` otherwise, where:
/// - `K_ij = k(||x_i - c_j||; length_scale, nu)` is the Matérn kernel block.
///
/// The default kernel penalty is `alpha' S alpha` with `S_jl = k(||c_j - c_l||)`, embedded
/// in the full coefficient space. With intercept included, that column is unpenalized by
/// `penalty_kernel`; optional `penalty_ridge` is the center-function-metric
/// penalty for double-penalty shrinkage of the explicit intercept direction.
///
/// NOTE: This follows the RKHS Gram construction S = K_CC (not K_CC^{-1}) in
/// coefficient space, with global scaling absorbed by the smoothing parameter λ.
pub fn create_matern_spline_basiswithworkspace(
    data: ArrayView2<'_, f64>,
    centers: ArrayView2<'_, f64>,
    length_scale: f64,
    nu: MaternNu,
    include_intercept: bool,
    aniso_log_scales: Option<&[f64]>,
    workspace: &mut BasisWorkspace,
) -> Result<MaternSplineBasis, BasisError> {
    let n = data.nrows();
    let d = data.ncols();
    let k = centers.nrows();
    let total_cols = k + usize::from(include_intercept);
    let dense_bytes = dense_design_bytes(n, total_cols);
    if dense_bytes > workspace.policy().max_single_materialization_bytes {
        crate::bail_invalid_basis!(
            "Matérn basis dense design exceeds resource policy: n={n}, p={total_cols}, dense={:.1} MiB, cap={:.1} MiB",
            dense_bytes as f64 / (1024.0 * 1024.0),
            workspace.policy().max_single_materialization_bytes as f64 / (1024.0 * 1024.0),
        );
    }

    if d == 0 {
        crate::bail_invalid_basis!("Matérn basis requires at least one covariate dimension");
    }
    if k == 0 {
        crate::bail_invalid_basis!("Matérn basis requires at least one center");
    }
    if centers.ncols() != d {
        crate::bail_dim_basis!(
            "Matérn basis dimension mismatch: data has {d} columns, centers have {}",
            centers.ncols()
        );
    }
    if data.iter().any(|v| !v.is_finite()) || centers.iter().any(|v| !v.is_finite()) {
        crate::bail_invalid_basis!("Matérn basis requires finite data and center values");
    }
    validate_matern_length_scale(length_scale)?;
    if let Some(eta) = aniso_log_scales {
        if eta.len() != d {
            crate::bail_dim_basis!(
                "aniso_log_scales length {} does not match data dimension {d}",
                eta.len()
            );
        }
        if eta.iter().any(|v| !v.is_finite()) {
            crate::bail_invalid_basis!("aniso_log_scales must contain finite values");
        }
    }

    // Practical safe operating range for κ from center geometry (document Eq. D.2):
    //   κ in [1e-2 / r_max, 1e2 / r_min], with κ = 1/length_scale.
    // Warn rather than silently clamp so callers keep explicit control.
    // Under anisotropy the kernel metric is y-space (y_a = exp(η_a) x_a), so
    // the relevant r_min/r_max are y-space pairwise distances, not raw.
    let warn_bounds = if let Some(eta) = aniso_log_scales {
        let y_centers = points_in_aniso_y_space(centers, eta);
        pairwise_distance_bounds(y_centers.view())
    } else {
        pairwise_distance_bounds(centers)
    };
    if let Some((r_min, r_max)) = warn_bounds {
        let kappa = 1.0 / length_scale.max(1e-300);
        let kappa_lo = 1e-2 / r_max;
        let kappa_hi = 1e2 / r_min;
        if kappa < kappa_lo || kappa > kappa_hi {
            log::debug!(
                "Matérn κ={} is outside recommended range [{}, {}] derived from centers (r_min={}, r_max={}); kernel conditioning may degrade",
                kappa,
                kappa_lo,
                kappa_hi,
                r_min,
                r_max
            );
        }
    }

    // Distance computation: anisotropic when eta is present, isotropic otherwise.
    // Under anisotropy we work in y-space (y = Ax), so r = |Ah| replaces |h|.
    let mut kernel_block = Array2::<f64>::zeros((n, k));
    let mut center_kernel = Array2::<f64>::zeros((k, k));
    let axis_scales = aniso_log_scales.map(aniso_axis_scales);
    let kernel_result: Result<(), BasisError> = kernel_block
        .axis_iter_mut(Axis(0))
        .into_par_iter()
        .enumerate()
        .try_for_each(|(i, mut row)| {
            for j in 0..k {
                let r = if let Some(scales) = axis_scales.as_deref() {
                    aniso_distance_rows_with_scales(data, i, centers, j, scales)
                } else {
                    euclidean_distance_rows(data, i, centers, j)
                };
                row[j] = matern_kernel_from_distance(r, length_scale, nu)?;
            }
            Ok(())
        });
    kernel_result?;
    // Center-center Gram matrix K_CC. In RKHS form, the kernel penalty on
    // radial coefficients is alpha^T K_CC alpha.
    fill_symmetric_from_row_kernel(&mut center_kernel, |i, j| {
        let r = if let Some(scales) = axis_scales.as_deref() {
            aniso_distance_rows_with_scales(centers, i, centers, j, scales)
        } else {
            euclidean_distance_rows(centers, i, centers, j)
        };
        matern_kernel_from_distance(r, length_scale, nu)
    })?;

    let mut basis = Array2::<f64>::zeros((n, total_cols));
    basis.slice_mut(s![.., 0..k]).assign(&kernel_block);
    if include_intercept {
        basis.column_mut(k).fill(1.0);
    }

    let mut penalty_kernel = Array2::<f64>::zeros((total_cols, total_cols));
    // RKHS coefficient penalty uses the center Gram matrix directly:
    //   S = K_CC  (not K_CC^{-1}).
    // This matches Duchon/Matérn spline theory where alpha^T K_CC alpha is the
    // native-space quadratic form up to a global scaling absorbed by lambda.
    penalty_kernel
        .slice_mut(s![0..k, 0..k])
        .assign(&center_kernel);
    let function_gram = matern_center_function_gram(&penalty_kernel, include_intercept, None)?;
    let penalty_ridge = if include_intercept {
        let mut intercept_frame = Array2::<f64>::zeros((total_cols, 1));
        intercept_frame[[total_cols - 1, 0]] = 1.0;
        function_space_subspace_shrinkage(&intercept_frame, &function_gram)?
    } else {
        Array2::<f64>::zeros((total_cols, total_cols))
    };

    Ok(MaternSplineBasis {
        basis,
        penalty_kernel,
        penalty_ridge,
        num_kernel_basis: k,
        num_polynomial_basis: usize::from(include_intercept),
        dimension: d,
    })
}

#[inline]
pub(crate) fn validate_lat_lon_matrix(
    data: ArrayView2<'_, f64>,
    context: &str,
    radians: bool,
) -> Result<(), BasisError> {
    if data.ncols() != 2 {
        crate::bail_dim_basis!(
            "{context} requires exactly two columns: latitude and longitude; got {}",
            data.ncols()
        );
    }
    if data.nrows() == 0 {
        crate::bail_invalid_basis!("{context} requires at least one row");
    }
    let (lat_lo, lat_hi, unit) = if radians {
        (
            -std::f64::consts::FRAC_PI_2,
            std::f64::consts::FRAC_PI_2,
            "radians",
        )
    } else {
        (-90.0, 90.0, "degrees")
    };
    for (i, row) in data.outer_iter().enumerate() {
        let lat = row[0];
        let lon = row[1];
        if !lat.is_finite() || !lon.is_finite() {
            crate::bail_invalid_basis!(
                "{context} requires finite latitude/longitude; row {i} has ({lat}, {lon})"
            );
        }
        if !(lat_lo..=lat_hi).contains(&lat) {
            crate::bail_invalid_basis!(
                "{context} latitude must be in [{lat_lo}, {lat_hi}] {unit}; row {i} has {lat}"
            );
        }
    }
    Ok(())
}

fn validate_spherical_wahba_gram_request(
    penalty_order: usize,
    kernel: SphereWahbaKernel,
) -> Result<(), BasisError> {
    if !(1..=4).contains(&penalty_order) {
        crate::bail_invalid_basis!(
            "spherical spline penalty_order must be one of 1, 2, 3, 4; got {penalty_order}"
        );
    }
    if matches!(kernel, SphereWahbaKernel::Sobolev) && penalty_order == 1 {
        // K_1 = (-ln(u) - 1)/(4π), u = (1 - cos(γ))/2, is log-singular
        // at coincidence. A finite Gram diagonal therefore cannot be inferred
        // from this closed form: the old epsilon floor silently selected one,
        // equivalent to an unstated spectral resolution of about 3.8e9.
        crate::bail_invalid_basis!(
            "the m = 1 Sobolev sphere kernel is log-singular at coincident points, so its Gram \
             diagonal does not exist and any finite value is a choice of resolution rather than a \
             limit; use SobolevTruncated {{ lmax }} (the same kernel with the resolution stated, \
             diagonal ~ ln(lmax)/2pi) or penalty_order >= 2, whose diagonals are finite closed \
             forms (1/(4pi) at m = 2, (2*zeta3 - 2)/(4pi) at m = 3)"
        );
    }
    Ok(())
}

/// Build a Wahba S² kernel matrix with the untruncated Sobolev kernel.
///
/// Untruncated Sobolev `m = 1` is refused because its coincident-point value
/// diverges; use [`SphereWahbaKernel::SobolevTruncated`] with
/// [`spherical_wahba_kernel_matrix_with_kind`] to state a finite resolution.
pub fn spherical_wahba_kernel_matrix(
    data: ArrayView2<'_, f64>,
    centers: ArrayView2<'_, f64>,
    penalty_order: usize,
    radians: bool,
) -> Result<Array2<f64>, BasisError> {
    spherical_wahba_kernel_matrix_with_kind(
        data,
        centers,
        penalty_order,
        radians,
        SphereWahbaKernel::Sobolev,
    )
}

/// Build a Wahba S² kernel matrix with an explicit kernel family.
///
/// Untruncated [`SphereWahbaKernel::Sobolev`] at `m = 1` is refused before
/// either GPU dispatch or CPU scalar/SIMD evaluation. Its Gram diagonal does
/// not exist; [`SphereWahbaKernel::SobolevTruncated`] is the explicit-
/// resolution alternative.
pub fn spherical_wahba_kernel_matrix_with_kind(
    data: ArrayView2<'_, f64>,
    centers: ArrayView2<'_, f64>,
    penalty_order: usize,
    radians: bool,
    kernel: SphereWahbaKernel,
) -> Result<Array2<f64>, BasisError> {
    validate_spherical_wahba_gram_request(penalty_order, kernel)?;
    validate_lat_lon_matrix(data, "spherical spline data", radians)?;
    validate_lat_lon_matrix(centers, "spherical spline centers", radians)?;
    // GPU fast path for the truncated-spectral kernels. The CPU SIMD loop
    // (`spherical_wahba_kernel_matrix_cpu`) is the bit-defining oracle; the
    // device only engages when `sphere_kernel_decision` admits the work (large
    // `n·m`, `lmax ≤ 200`, memory budget). `None` ⇒ quiet CPU route (closed-form
    // variant, no device, or below threshold); `Some(Err)` ⇒ admitted device
    // failed ⇒ surface it (never a silent CPU degrade — the engagement-failure
    // class this path kills).
    if let Some(gpu_result) = crate::basis::sphere_gpu::try_build_truncated_kernel_matrix_gpu(
        data,
        centers,
        penalty_order,
        radians,
        kernel,
    ) {
        let gpu_matrix = gpu_result.map_err(|err| {
            BasisError::InvalidInput(format!(
                "spherical spline GPU truncated kernel was admitted but failed on device: {err}"
            ))
        })?;
        return Ok(gpu_matrix);
    }
    spherical_wahba_kernel_matrix_cpu_validated(data, centers, penalty_order, radians, kernel)
}

/// CPU oracle for the Wahba S² kernel design matrix — the bit-defining
/// reference the GPU truncated path is held to. Always evaluates on host,
/// regardless of the GPU dispatch decision, so parity tests and any caller that
/// needs the deterministic reference can bypass device routing entirely.
///
/// It enforces the same kernel/order contract as
/// [`spherical_wahba_kernel_matrix_with_kind`]; bypassing device routing does
/// not bypass mathematical validation.
pub fn spherical_wahba_kernel_matrix_cpu(
    data: ArrayView2<'_, f64>,
    centers: ArrayView2<'_, f64>,
    penalty_order: usize,
    radians: bool,
    kernel: SphereWahbaKernel,
) -> Result<Array2<f64>, BasisError> {
    validate_spherical_wahba_gram_request(penalty_order, kernel)?;
    validate_lat_lon_matrix(data, "spherical spline data", radians)?;
    validate_lat_lon_matrix(centers, "spherical spline centers", radians)?;
    spherical_wahba_kernel_matrix_cpu_validated(data, centers, penalty_order, radians, kernel)
}

fn spherical_wahba_kernel_matrix_cpu_validated(
    data: ArrayView2<'_, f64>,
    centers: ArrayView2<'_, f64>,
    penalty_order: usize,
    radians: bool,
    kernel: SphereWahbaKernel,
) -> Result<Array2<f64>, BasisError> {
    let n = data.nrows();
    let k = centers.nrows();
    let deg = if radians {
        1.0
    } else {
        std::f64::consts::PI / 180.0
    };
    // Precompute (sin_lat, cos_lat, sin_lon, cos_lon) for each center once and
    // reuse it across the whole N x K grid. The pair separation is then pure
    // `+ - *` arithmetic on those eight numbers — see
    // `super::sphere_half_angle` for why it is taken in chord form rather than
    // as a dot product (#2489) and why it costs no transcendental call per
    // (i, j) either way.
    let mut sin_lat_c = Vec::<f64>::with_capacity(k);
    let mut cos_lat_c = Vec::<f64>::with_capacity(k);
    let mut sin_lon_c = Vec::<f64>::with_capacity(k);
    let mut cos_lon_c = Vec::<f64>::with_capacity(k);
    for c in centers.outer_iter() {
        let trig = SphereTrig::from_radians(c[0] * deg, c[1] * deg);
        sin_lat_c.push(trig.sin_lat);
        cos_lat_c.push(trig.cos_lat);
        sin_lon_c.push(trig.sin_lon);
        cos_lon_c.push(trig.cos_lon);
    }
    let mut out = Array2::<f64>::zeros((n, k));
    let err_flag = std::sync::atomic::AtomicBool::new(false);
    out.axis_chunks_iter_mut(ndarray::Axis(0), 256)
        .into_par_iter()
        .enumerate()
        .for_each(|(chunk_idx, mut block)| {
            use wide::f64x4;
            let row_offset = chunk_idx * 256;
            let chunks = k / 4;
            let tail = k % 4;
            for (local_i, mut out_row) in block.outer_iter_mut().enumerate() {
                let i = row_offset + local_i;
                let row = SphereTrig::from_radians(data[(i, 0)] * deg, data[(i, 1)] * deg);
                let row_v = SphereTrig {
                    sin_lat: f64x4::from(row.sin_lat),
                    cos_lat: f64x4::from(row.cos_lat),
                    sin_lon: f64x4::from(row.sin_lon),
                    cos_lon: f64x4::from(row.cos_lon),
                };
                // SIMD over 4 centers at a time.
                for cidx in 0..chunks {
                    let base = cidx * 4;
                    let center_v = SphereTrig {
                        sin_lat: f64x4::from([
                            sin_lat_c[base],
                            sin_lat_c[base + 1],
                            sin_lat_c[base + 2],
                            sin_lat_c[base + 3],
                        ]),
                        cos_lat: f64x4::from([
                            cos_lat_c[base],
                            cos_lat_c[base + 1],
                            cos_lat_c[base + 2],
                            cos_lat_c[base + 3],
                        ]),
                        sin_lon: f64x4::from([
                            sin_lon_c[base],
                            sin_lon_c[base + 1],
                            sin_lon_c[base + 2],
                            sin_lon_c[base + 3],
                        ]),
                        cos_lon: f64x4::from([
                            cos_lon_c[base],
                            cos_lon_c[base + 1],
                            cos_lon_c[base + 2],
                            cos_lon_c[base + 3],
                        ]),
                    };
                    let (u, v) = half_angle_separation(row_v, center_v);
                    let vals = wahba_sphere_kernel_simd_kind(u, v, penalty_order, kernel);
                    let arr = vals.to_array();
                    for lane in 0..4 {
                        if !arr[lane].is_finite() {
                            err_flag.store(true, std::sync::atomic::Ordering::Relaxed);
                            return;
                        }
                        out_row[base + lane] = arr[lane];
                    }
                }
                // Scalar tail (0..3 elements).
                let tail_start = chunks * 4;
                for t in 0..tail {
                    let j = tail_start + t;
                    let center = SphereTrig {
                        sin_lat: sin_lat_c[j],
                        cos_lat: cos_lat_c[j],
                        sin_lon: sin_lon_c[j],
                        cos_lon: cos_lon_c[j],
                    };
                    let sep = half_angle_separation_scalar(row, center);
                    match wahba_sphere_kernel_kind(sep, penalty_order, kernel) {
                        Ok(v) => out_row[j] = v,
                        Err(_) => {
                            err_flag.store(true, std::sync::atomic::Ordering::Relaxed);
                            return;
                        }
                    }
                }
            }
        });
    if err_flag.load(std::sync::atomic::Ordering::Relaxed) {
        crate::bail_invalid_basis!("spherical spline kernel produced a non-finite value");
    }
    Ok(out)
}

#[cfg(test)]
mod spherical_wahba_kernel_contract_2475_tests {
    use super::*;
    use ndarray::array;

    fn assert_sobolev_m1_refusal(entry_point: &str, result: Result<Array2<f64>, BasisError>) {
        let error = result.expect_err("untruncated Sobolev m=1 has no Gram diagonal");
        let message = error.to_string();
        assert!(
            message.contains("log-singular") && message.contains("SobolevTruncated"),
            "{entry_point} must identify both the mathematical defect and the explicit-resolution \
             remedy; got: {message}"
        );
    }

    #[test]
    fn all_public_matrix_entry_points_refuse_untruncated_sobolev_m1() {
        // Deliberately use distinct points. Refusal is a structural property of
        // the requested Gram-kernel family, not a floating-point coincidence test.
        let data = array![[0.0, 0.0]];
        let centers = array![[35.0, 70.0]];

        assert_sobolev_m1_refusal(
            "spherical_wahba_kernel_matrix",
            spherical_wahba_kernel_matrix(data.view(), centers.view(), 1, false),
        );
        assert_sobolev_m1_refusal(
            "spherical_wahba_kernel_matrix_with_kind",
            spherical_wahba_kernel_matrix_with_kind(
                data.view(),
                centers.view(),
                1,
                false,
                SphereWahbaKernel::Sobolev,
            ),
        );
        assert_sobolev_m1_refusal(
            "spherical_wahba_kernel_matrix_cpu",
            spherical_wahba_kernel_matrix_cpu(
                data.view(),
                centers.view(),
                1,
                false,
                SphereWahbaKernel::Sobolev,
            ),
        );
    }

    #[test]
    fn explicit_resolution_and_finite_diagonal_m1_kernels_remain_available() {
        let point = array![[0.0, 0.0]];

        let pseudo = spherical_wahba_kernel_matrix_with_kind(
            point.view(),
            point.view(),
            1,
            false,
            SphereWahbaKernel::Pseudo,
        )
        .expect("pseudo-Wahba m=1 has a finite analytic coincident-point value");
        assert_eq!(
            pseudo[(0, 0)],
            1.0 / (4.0 * std::f64::consts::PI),
            "the refusal must not absorb valid pseudo-Wahba m=1"
        );

        let truncated = spherical_wahba_kernel_matrix_with_kind(
            point.view(),
            point.view(),
            1,
            false,
            SphereWahbaKernel::SobolevTruncated { lmax: 16 },
        )
        .expect("explicitly truncated Sobolev m=1 has a stated finite resolution");
        assert!(
            truncated[(0, 0)].is_finite(),
            "a stated spectral resolution must produce a finite Gram diagonal"
        );

        spherical_wahba_kernel_matrix(point.view(), point.view(), 2, false)
            .expect("untruncated Sobolev m=2 has a finite closed-form diagonal");
    }
}

pub(crate) fn weighted_coefficient_sum_to_zero_transform(
    weights: ArrayView1<'_, f64>,
) -> Result<Array2<f64>, BasisError> {
    let k = weights.len();
    if k < 2 {
        return Err(BasisError::InsufficientColumnsForConstraint { found: k });
    }
    if weights.iter().any(|w| !w.is_finite() || *w < 0.0) {
        crate::bail_invalid_basis!(
            "sphere coefficient constraint weights must be finite and non-negative"
        );
    }
    let norm = weights.iter().map(|w| w * w).sum::<f64>().sqrt();
    if norm <= 0.0 {
        crate::bail_invalid_basis!("sphere coefficient constraint weights cannot all be zero");
    }
    let c = Array2::from_shape_vec((k, 1), weights.iter().map(|w| *w / norm).collect())
        .map_err(|e| BasisError::InvalidInput(format!("invalid sphere constraint weights: {e}")))?;
    let (z, rank) =
        rrqr_nullspace_basis(&c, default_rrqr_rank_alpha()).map_err(BasisError::LinalgError)?;
    if rank >= k {
        return Err(BasisError::ConstraintNullspaceCollapsed {
            site: "weighted_coefficient_sum_to_zero_transform",
            cross_rank: rank,
            coeff_dim: k,
            cross_frobenius: 1.0,
            gram_spectrum: "not computed (structural rank collapse before Gram eigendecomposition)"
                .to_string(),
        });
    }
    Ok(z)
}

const SPHERICAL_CENTER_COINCIDENT_TOL: f64 = 1.0e-12;

#[inline]
fn spherical_center_dot(a: &[f64; 3], b: &[f64; 3]) -> f64 {
    a[0] * b[0] + a[1] * b[1] + a[2] * b[2]
}

/// Reduce a candidate list that is already tied on every `O(1)` invariant key to
/// the sub-list attaining the lexicographically least sorted **dot** profile —
/// the multiset `{uᵢ·u_j : j}` of one row against the whole cloud, in ascending
/// total order. Rows related by a rotation that maps the point cloud to itself
/// have the SAME profile, which is what makes it a legal tie-break key: it
/// depends on neither the frame nor the row order.
///
/// The tie-break machinery itself — extremum-then-refine, one `O(n log n)`
/// profile per candidate serving both the choice and the class filter, none at
/// all for a lone candidate — is shared with the Euclidean twin
/// ([`select_thin_plate_knots`]) in [`crate::basis::invariant_tie_break`]. Only
/// the pairwise scalar differs: a dot product here, a squared distance there.
fn resolve_spherical_profile_tie<F>(
    units: &[[f64; 3]],
    tied: &[usize],
    on_profile_builds: &mut F,
) -> Vec<usize>
where
    F: FnMut(usize),
{
    resolve_sorted_profile_tie(
        units.len(),
        tied,
        |anchor, row| spherical_center_dot(&units[anchor], &units[row]),
        on_profile_builds,
    )
}

/// Remove coincident directions from one invariant tie class without choosing
/// between genuinely distinct tied directions. Representatives of coincident
/// rows are geometrically interchangeable and produce the same kernel column;
/// every distinct member of the symmetry class is retained.
fn distinct_spherical_orbit(
    units: &[[f64; 3]],
    candidates: &[usize],
    already_selected: &[usize],
) -> Vec<usize> {
    let mut distinct = Vec::with_capacity(candidates.len());
    'candidate: for &candidate in candidates {
        for &selected in already_selected.iter().chain(distinct.iter()) {
            if spherical_center_dot(&units[candidate], &units[selected])
                >= 1.0 - SPHERICAL_CENTER_COINCIDENT_TOL
            {
                continue 'candidate;
            }
        }
        distinct.push(candidate);
    }
    distinct
}

/// Select spherical-spline basis centers by **geodesic** farthest-point sampling
/// of the data cloud, returning a well-spread subset of the actual data rows.
///
/// This is the rotation-EQUIVARIANT center rule Wahba's reproducing-kernel smooth
/// needs. The kernel is a function of the geodesic angle alone (`k(cos γ)`,
/// `cos γ = uᵢ·u_c` for unit vectors `u`), so the continuous estimator is exactly
/// SO(3)-invariant; the finite-center discretization inherits that invariance
/// **iff** the centers rotate rigidly with the data. Every ingredient of this
/// selection is a dot product of data unit vectors — the mean-direction seed key
/// `uᵢ·Σⱼuⱼ`, the maximin nearest-center dot `max_c uᵢ·u_c`, and the sorted
/// dot-profile tie-break — and a dot product is invariant under any rotation `R`
/// (`(Ruᵢ)·(Ru_c) = uᵢ·u_c`). So under ANY rotation of the data the SAME physical
/// rows are selected, the returned centers are exactly those rows rotated, every
/// kernel entry `k(uᵢ·u_c)` is preserved, and the fit and every prediction are
/// invariant to the arbitrary choice of frame (a longitude origin, a tilt, any
/// element of SO(3)) — matching the rotation-invariant `harmonic` control (#2127).
///
/// On a symmetric cloud, invariant scalar keys can leave several **distinct**
/// rows exactly tied. No row-permutation-equivariant rule can choose one member
/// of such an orbit: a symmetry exchanging two tied rows would have to both
/// preserve and change that choice. The selector therefore adds the complete
/// distinct-direction tie class atomically. Because `num_centers` is an exact
/// resource contract, a class that does not fit in the remaining budget is
/// refused as unrepresentable rather than truncated by row index. Coincident
/// rows remain one kernel column; consequently a request exceeding the number
/// of distinct directions is also refused rather than silently undersized.
///
/// The previous implementation ignored `data` and laid down a fixed golden-angle
/// (Fibonacci) lattice pinned in the (lat, lon) frame: a rigid rotation moved the
/// data relative to the STATIONARY centers, changed every data-to-center geodesic
/// angle, and reshaped the fitted surface. Anchoring only the lattice's longitude
/// origin to the data (a first pass at #2127) fixed rotations about the pole but
/// left the frame-pinned latitudes exposed to a tilt.
///
/// The selection mirrors the Euclidean thin-plate knot picker
/// ([`select_thin_plate_knots`]) — centroid-nearest seed, maximin recursion,
/// invariant tie-breaks — but with geodesic (great-circle) distance in place of
/// Euclidean distance, which is the correct SO(3) invariant on S². Coincident
/// data directions are not selected twice (a duplicate center makes the Wahba
/// Gram singular).
///
/// Each step minimizes its composite key in extremum-then-refine order rather
/// than by carrying a running incumbent: the two `O(1)` keys in one parallel
/// reduction, then the rows attaining them in one parallel filter, then — only
/// over that set, and only if it holds more than one row — the `O(n log n)`
/// sorted dot profile. Lexicographic minimization is associative, so this is the
/// same total preorder the incumbent scan applied; what changes is that the
/// profile key is charged where it can still decide something instead of twice
/// per outer iteration whether or not anything is tied. On data with no exact
/// spherical symmetry it is never built at all (#2420).
pub fn select_spherical_farthest_point_centers(
    data: ArrayView2<'_, f64>,
    num_centers: usize,
    radians: bool,
) -> Result<Array2<f64>, BasisError> {
    let chosen = select_spherical_farthest_point_center_rows(data, num_centers, radians)?;
    log::debug!(
        "spherical farthest-point centers: {} of {} rows, {} sorted dot profile(s) built",
        chosen.rows.len(),
        data.nrows(),
        chosen.profile_builds
    );
    // Return the selected rows VERBATIM (in the data's own lat/lon units), so
    // the centers ARE data points and carry the rotation exactly.
    Ok(Array2::from_shape_fn((chosen.rows.len(), 2), |(r, c)| {
        data[[chosen.rows[r], c]]
    }))
}

/// The row indices [`select_spherical_farthest_point_centers`] selects, with
/// the number of sorted dot profiles the selection had to build.
pub(crate) struct SphericalCenterSelection {
    pub(crate) rows: Vec<usize>,
    /// How many `O(n log n)` sorted dot profiles the tie-break machinery built.
    /// Zero whenever no invariant tie ever had more than one candidate — the
    /// property the extremum-then-refine order exists to guarantee (#2420) —
    /// so it is reported rather than observed through a callback.
    pub(crate) profile_builds: usize,
}

fn select_spherical_farthest_point_center_rows(
    data: ArrayView2<'_, f64>,
    num_centers: usize,
    radians: bool,
) -> Result<SphericalCenterSelection, BasisError> {
    use rayon::prelude::*;
    let mut profile_builds = 0usize;
    validate_lat_lon_matrix(data, "spherical farthest-point centers", radians)?;
    if num_centers == 0 {
        crate::bail_invalid_basis!("spherical farthest-point center count must be positive");
    }
    let n = data.nrows();
    if n < 2 {
        return Err(BasisError::InsufficientColumnsForConstraint { found: n });
    }
    if num_centers > n {
        crate::bail_invalid_basis!(
            "requested {num_centers} spherical farthest-point centers but only {n} rows are available"
        );
    }

    let to_rad = if radians {
        1.0
    } else {
        std::f64::consts::PI / 180.0
    };
    // Unit vectors on S² for each data row. The geodesic distance between rows is
    // a monotone-DECREASING function of the dot product `uᵢ·uⱼ = cos γ`, so every
    // "distance" comparison below is phrased directly in dot products — each of
    // which is exactly rotation invariant.
    let units: Vec<[f64; 3]> = (0..n)
        .into_par_iter()
        .map(|i| {
            let lat = data[[i, 0]] * to_rad;
            let lon = data[[i, 1]] * to_rad;
            let cos_lat = lat.cos();
            [cos_lat * lon.cos(), cos_lat * lon.sin(), lat.sin()]
        })
        .collect();
    // Mean-direction seed key `dot_to_sum[i] = uᵢ·Σⱼuⱼ`. `Σⱼuⱼ` is
    // rotation-EQUIVARIANT (it rotates rigidly with the data), so `argmax` is the
    // SAME physical row in every frame. Using the UNNORMALIZED resultant avoids
    // the fp blow-up of normalizing a near-zero mean direction on a well-covered
    // sphere (`dot_to_sum` is a homogeneous linear function of the resultant, so
    // its relative accuracy — and hence the argmax — is stable regardless of the
    // resultant's magnitude). Each component sum is taken in value-sorted order so
    // the key is also invariant to a pure row permutation (matching
    // `select_thin_plate_knots`).
    let mut sum = [0.0_f64; 3];
    for (c, sum_c) in sum.iter_mut().enumerate() {
        let mut col: Vec<f64> = units.par_iter().map(|u| u[c]).collect();
        // Sorted in parallel but summed sequentially: the value-sorted ORDER is
        // what makes the key permutation invariant, and the accumulation must
        // stay left-to-right over that order to keep the sum bit-reproducible.
        col.par_sort_by(|a, b| a.total_cmp(b));
        *sum_c = col.iter().sum();
    }
    let dot_to_sum: Vec<f64> = units
        .par_iter()
        .map(|u| spherical_center_dot(u, &sum))
        .collect();

    // Seed class = rows nearest the mean direction (largest `dot_to_sum`), then
    // lexicographically smallest intrinsic dot profile. If that complete key is
    // tied, retain the whole symmetry orbit; a row-index tie-break is forbidden.
    // Both keys are minimized in extremum-then-refine order, so the `O(n log n)`
    // profile key is built only for rows that survive the `O(1)` one — none at
    // all when the mean-direction argmax is unique (#2420).
    let seed_key = dot_to_sum.par_iter().copied().reduce(
        || f64::NEG_INFINITY,
        |a, b| if b.total_cmp(&a).is_gt() { b } else { a },
    );
    let seed_tied: Vec<usize> = (0..n)
        .into_par_iter()
        .filter(|&i| dot_to_sum[i].total_cmp(&seed_key).is_eq())
        .collect();

    let target = num_centers;
    let seed_class = resolve_spherical_profile_tie(&units, &seed_tied, &mut |built: usize| {
        profile_builds += built;
    });
    let seed_orbit = distinct_spherical_orbit(&units, &seed_class, &[]);
    if seed_orbit.len() > target {
        crate::bail_invalid_basis!(
            "spherical farthest-point seed symmetry orbit has {} distinct directions, exceeding the requested center budget {target}; use a budget at least as large as the orbit or the harmonic sphere basis",
            seed_orbit.len()
        );
    }

    let mut selected = Vec::with_capacity(target);
    let mut chosen = vec![false; n];
    // `max_dot[i]` = `max` over chosen centers `c` of `uᵢ·u_c` = `cos` of the
    // geodesic distance to the NEAREST chosen center. The maximin step picks the
    // unchosen row MINIMIZING it (farthest from all chosen).
    let mut max_dot = vec![f64::NEG_INFINITY; n];
    for &i in &seed_class {
        chosen[i] = true;
    }
    selected.extend(seed_orbit);
    max_dot.par_iter_mut().enumerate().for_each(|(i, slot)| {
        *slot = selected
            .iter()
            .map(|&center| spherical_center_dot(&units[i], &units[center]))
            .fold(f64::NEG_INFINITY, f64::max);
    });

    // A dot `≥ 1 − SPHERICAL_CENTER_COINCIDENT_TOL` is a geodesic angle
    // `≲ 1.4e-6` rad: the
    // candidate coincides with an already-chosen center, so selecting it would add
    // a duplicate kernel column and a singular Wahba Gram. Stopping here caps the
    // center set at the number of DISTINCT data directions.
    while selected.len() < target {
        // Maximin: prefer the larger geodesic distance to the chosen set (the
        // SMALLER `max_dot`). Exact `max_dot` ties — common on symmetric clouds
        // and in float arithmetic — break first toward the MORE PERIPHERAL row
        // (smaller `dot_to_sum`, which spreads centers outward and is rotation
        // invariant), then by the invariant dot-profile. A tie after all three
        // keys is a symmetry orbit and is completed atomically below.
        //
        // The composite key is minimized in extremum-then-refine order rather
        // than by a running incumbent: one parallel reduction for the two `O(1)`
        // keys, one parallel filter for the rows attaining them, and the
        // `O(n log n)` profile key only over THAT set. The set is also exactly the
        // tie-class filter's candidate set, so the profiles are built once and
        // serve both. A unique maximin winner therefore builds no profile at all,
        // where the incumbent scan built two per outer iteration — one for the
        // winner and one to compare the winner against itself (#2420).
        let cheap_key = (0..n)
            .into_par_iter()
            .filter(|&i| !chosen[i])
            .map(|i| (max_dot[i], dot_to_sum[i]))
            .reduce(
                || (f64::INFINITY, f64::INFINITY),
                |a, b| {
                    if b.0.total_cmp(&a.0).then(b.1.total_cmp(&a.1)).is_lt() {
                        b
                    } else {
                        a
                    }
                },
            );
        let cheap_tied: Vec<usize> = (0..n)
            .into_par_iter()
            .filter(|&i| {
                !chosen[i]
                    && max_dot[i].total_cmp(&cheap_key.0).is_eq()
                    && dot_to_sum[i].total_cmp(&cheap_key.1).is_eq()
            })
            .collect();
        if cheap_tied.is_empty() {
            break;
        }
        if cheap_key.0 >= 1.0 - SPHERICAL_CENTER_COINCIDENT_TOL {
            break;
        }

        let tied_class = resolve_spherical_profile_tie(&units, &cheap_tied, &mut |built: usize| {
            profile_builds += built;
        });
        let orbit = distinct_spherical_orbit(&units, &tied_class, &selected);
        let remaining = target - selected.len();
        if orbit.len() > remaining {
            crate::bail_invalid_basis!(
                "spherical farthest-point tie class has {} distinct directions but only {remaining} of the exact {target}-center budget remain; choose a compatible center count or the harmonic sphere basis",
                orbit.len(),
            );
        }
        for &i in &tied_class {
            chosen[i] = true;
        }
        if orbit.is_empty() {
            continue;
        }
        selected.extend(orbit.iter().copied());
        let chosen_ref = &chosen;
        let orbit_ref = &orbit;
        max_dot.par_iter_mut().enumerate().for_each(|(i, slot)| {
            if chosen_ref[i] {
                return;
            }
            for &center in orbit_ref {
                let d = spherical_center_dot(&units[i], &units[center]);
                if d > *slot {
                    *slot = d;
                }
            }
        });
    }

    if selected.len() < target {
        crate::bail_invalid_basis!(
            "requested {target} distinct spherical farthest-point centers but the data contain only {} numerically distinct directions",
            selected.len()
        );
    }
    if selected.len() < 2 {
        return Err(BasisError::InsufficientColumnsForConstraint {
            found: selected.len(),
        });
    }

    Ok(SphericalCenterSelection {
        rows: selected,
        profile_builds,
    })
}

#[cfg(test)]
mod spherical_farthest_point_symmetry_tests {
    use super::*;
    use ndarray::{Array2, array};

    fn permute_rows(data: &Array2<f64>, order: &[usize]) -> Array2<f64> {
        Array2::from_shape_fn((order.len(), 2), |(row, col)| data[[order[row], col]])
    }

    fn sorted_center_rows(centers: &Array2<f64>) -> Vec<[f64; 2]> {
        let mut rows: Vec<[f64; 2]> = centers.outer_iter().map(|row| [row[0], row[1]]).collect();
        rows.sort_by(|a, b| a[0].total_cmp(&b[0]).then(a[1].total_cmp(&b[1])));
        rows
    }

    /// The equatorial point is the unique centroid-nearest seed. North and
    /// south are then exactly tied by every intrinsic key and are exchanged by
    /// a data symmetry, so selecting either one by row index is impossible to
    /// reconcile with permutation invariance. The selector must add both as one
    /// atomic orbit. A duplicate equatorial row remains one kernel column.
    #[test]
    fn symmetric_tie_orbit_is_completed_under_every_row_permutation() {
        let data = array![[0.0_f64, 0.0], [0.0, 0.0], [90.0, 0.0], [-90.0, 0.0]];
        let permutations = [[0_usize, 1, 2, 3], [0, 1, 3, 2], [2, 0, 3, 1], [3, 1, 2, 0]];

        let mut reference: Option<Vec<[f64; 2]>> = None;
        for order in permutations {
            let permuted = permute_rows(&data, &order);
            let centers = select_spherical_farthest_point_centers(permuted.view(), 3, false)
                .expect("the complete three-direction symmetry orbit is representable");
            assert_eq!(
                centers.nrows(),
                3,
                "the exact three-center target must contain the complete north/south tie class"
            );
            let center_set = sorted_center_rows(&centers);
            if let Some(expected) = &reference {
                assert_eq!(
                    &center_set, expected,
                    "selected physical center set changed under row permutation"
                );
            } else {
                reference = Some(center_set);
            }
        }
    }

    #[test]
    fn incomplete_nonseed_tie_class_is_refused() {
        let data = array![[0.0_f64, 0.0], [0.0, 0.0], [90.0, 0.0], [-90.0, 0.0]];
        let error = select_spherical_farthest_point_centers(data.view(), 2, false)
            .expect_err("one remaining slot cannot split the north/south tie class");
        assert!(
            error
                .to_string()
                .contains("only 1 of the exact 2-center budget remain"),
            "unexpected refusal: {error}"
        );
    }

    /// A symmetry orbit is indivisible. If even one orbit is larger than the
    /// declared resource budget, refusing is the only bounded equivariant
    /// answer; silently choosing a row-index representative is mathematically
    /// false and expanding without a bound can turn an O(m) request into O(n).
    #[test]
    fn symmetry_orbit_larger_than_center_budget_is_refused() {
        let antipodal = array![[90.0_f64, 0.0], [-90.0, 0.0]];
        let error = select_spherical_farthest_point_centers(antipodal.view(), 1, false)
            .expect_err("a two-direction seed orbit cannot fit a one-center budget");
        assert!(
            error.to_string().contains("symmetry orbit"),
            "unexpected refusal: {error}"
        );
    }

    /// The canonical gridded-geospatial layout, matching the `sphere_gpu`
    /// fixtures: latitude in (-85, 85), longitude spanning [-180, 180].
    fn latlon_grid(n_lat: usize, n_lon: usize) -> Array2<f64> {
        Array2::from_shape_fn((n_lat * n_lon, 2), |(row, col)| {
            let (i, j) = (row / n_lon, row % n_lon);
            if col == 0 {
                -85.0 + (170.0 * i as f64) / (n_lat.saturating_sub(1).max(1) as f64)
            } else {
                -180.0 + (360.0 * j as f64) / (n_lon.saturating_sub(1).max(1) as f64)
            }
        })
    }

    /// Deterministic area-uniform cloud: no exact spherical symmetry, so no two
    /// rows can tie the maximin key exactly.
    fn latlon_cloud(n: usize) -> Array2<f64> {
        let mut state = 0x2545_F491_4F6C_DD1D_u64;
        let mut next = move || {
            state ^= state << 13;
            state ^= state >> 7;
            state ^= state << 17;
            (state >> 11) as f64 / (1u64 << 53) as f64
        };
        let draws: Vec<f64> = (0..2 * n).map(|_| next()).collect();
        Array2::from_shape_fn((n, 2), |(row, col)| {
            if col == 0 {
                (1.0 - 2.0 * draws[2 * row]).asin().to_degrees()
            } else {
                360.0 * draws[2 * row + 1] - 180.0
            }
        })
    }

    /// The `O(n log n)` sorted dot profile is a tie-break, and a tie-break must
    /// only be paid for where something is actually tied. A cloud with no exact
    /// spherical symmetry has a unique maximin winner at every step, so the
    /// selection must complete having built NO profile at all — at any `n`, and
    /// for any center budget.
    ///
    /// The running-incumbent scan this replaced (#2420) built two profiles per
    /// outer iteration on exactly this input: one for the winner, and one to
    /// compare the winner against its own profile in the tie-class filter. At
    /// `m = 200` that was 400 sorts of `n` doubles to discover that nothing was
    /// tied, and it was 88% of the whole spherical basis build.
    #[test]
    fn spherical_center_selection_costs_no_profile_without_an_exact_tie() {
        for n in [2_000_usize, 8_000] {
            for m in [40_usize, 200] {
                let data = latlon_cloud(n);
                let chosen = select_spherical_farthest_point_center_rows(data.view(), m, false)
                    .expect("an asymmetric cloud admits any center budget below n");
                assert_eq!(chosen.rows.len(), m, "exact center budget (n={n}, m={m})");
                assert_eq!(
                    chosen.profile_builds, 0,
                    "no row can tie the maximin key exactly on an asymmetric cloud, so the \
                     profile tie-break must never be built (n={n}, m={m})"
                );
            }
        }
    }

    /// On a regular lat/lon grid the tie-break IS reached — a parallel's rows are
    /// genuinely related by a rotation about the polar axis. The cost of reaching
    /// it must still be a property of the symmetry, not of the row count: the
    /// profile key may only be built for rows that tie both `O(1)` keys at the
    /// maximin extremum, so the count stays below one profile per selected center
    /// even as `n` grows 16-fold. The scan this replaced built strictly more than
    /// two per center regardless of `n`.
    #[test]
    fn spherical_center_profile_cost_does_not_scale_with_the_row_count() {
        for (n_lat, n_lon) in [(40_usize, 40_usize), (160, 160)] {
            for m in [40_usize, 200] {
                let data = latlon_grid(n_lat, n_lon);
                let n = data.nrows();
                let chosen = select_spherical_farthest_point_center_rows(data.view(), m, false)
                    .expect("a lat/lon grid admits these center budgets");
                assert_eq!(chosen.rows.len(), m, "exact center budget (n={n}, m={m})");
                assert!(
                    chosen.profile_builds < m,
                    "profile-key builds must stay below one per selected center; got {} at \
                     n={n} m={m} (the replaced incumbent scan built at least {})",
                    chosen.profile_builds,
                    2 * m
                );
            }
        }
    }

    /// The gate above must not be satisfiable by deleting the tie-break. On the
    /// pole/equator fixture the profile key is what proves north and south are one
    /// indivisible orbit, so it must genuinely be built there.
    #[test]
    fn spherical_center_profile_key_is_still_built_where_it_decides_an_orbit() {
        let data = array![[0.0_f64, 0.0], [0.0, 0.0], [90.0, 0.0], [-90.0, 0.0]];
        let chosen = select_spherical_farthest_point_center_rows(data.view(), 3, false)
            .expect("the complete three-direction symmetry orbit is representable");
        assert!(
            chosen.profile_builds > 0,
            "the north/south orbit is only provable through the invariant profile key"
        );
    }

    /// Extremum-then-refine reaches the same physical answer as the incumbent
    /// scan it replaced only if the composite key is evaluated over the same
    /// candidate set. On two symmetric parallels every `max_dot` extremum is a
    /// multi-row tie, so the whole selection is decided inside the tie logic —
    /// and it must still be blind to row order at every budget.
    #[test]
    fn polar_ring_selection_is_row_order_blind_at_every_budget() {
        // Two parallels at ±30°, six points each.
        let ring: Vec<[f64; 2]> = [-30.0_f64, 30.0]
            .into_iter()
            .flat_map(|lat| (0..6).map(move |j| [lat, -180.0 + 60.0 * j as f64]))
            .collect();
        let data = Array2::from_shape_fn((ring.len(), 2), |(r, c)| ring[r][c]);
        let n = data.nrows();

        for budget in 2..=n {
            let reference = select_spherical_farthest_point_centers(data.view(), budget, false)
                .map(|centers| sorted_center_rows(&centers));
            for order in [
                (0..n).rev().collect::<Vec<usize>>(),
                (0..n).map(|i| (5 * i + 7) % n).collect::<Vec<usize>>(),
                (0..n)
                    .step_by(5)
                    .chain((1..n).step_by(5))
                    .collect::<Vec<usize>>(),
            ] {
                if order.len() != n {
                    continue;
                }
                let permuted = permute_rows(&data, &order);
                let got = select_spherical_farthest_point_centers(permuted.view(), budget, false)
                    .map(|centers| sorted_center_rows(&centers));
                match (&reference, &got) {
                    (Ok(expected), Ok(actual)) => assert_eq!(
                        actual, expected,
                        "budget {budget}: selected physical directions changed under a row \
                         permutation of a symmetric ring"
                    ),
                    (Err(a), Err(b)) => assert_eq!(
                        a.to_string(),
                        b.to_string(),
                        "budget {budget}: refusal changed under a row permutation"
                    ),
                    _ => panic!(
                        "budget {budget}: row order decided whether the request was \
                         representable ({reference:?} vs {got:?})"
                    ),
                }
            }
        }
    }
}

#[cfg(test)]
mod matern_function_metric_tests {
    use super::*;
    use ndarray::array;

    #[test]
    fn center_metric_null_ridge_is_covariant_and_targets_only_intercept_function() {
        let center_kernel = array![[1.4, 0.3, 0.1], [0.3, 1.2, 0.2], [0.1, 0.2, 1.1]];
        let mut embedded = Array2::<f64>::zeros((4, 4));
        embedded.slice_mut(s![0..3, 0..3]).assign(&center_kernel);
        let gram =
            matern_center_function_gram(&embedded, true, None).expect("raw center function Gram");
        let base =
            matern_double_penalty_candidates(&embedded, &gram, true).expect("raw candidates");
        assert_eq!(base.len(), 2);
        let raw_ridge = base[1].matrix.dense() * base[1].normalization_scale;

        let intercept = array![[0.0], [0.0], [0.0], [1.0]];
        let action_error = (&raw_ridge.dot(&intercept) - &gram.dot(&intercept))
            .iter()
            .map(|value| value.abs())
            .fold(0.0_f64, f64::max);
        assert!(
            action_error < 2.0e-13,
            "ridge must equal G on the structural intercept; error={action_error:.3e}"
        );

        // A strongly non-orthogonal kernel chart plus intercept rescaling. The
        // block structure is exactly Matérn's supported final transform: kernel
        // coordinates may shear/rescale, while the explicit intercept remains a
        // separate structural coordinate.
        let transform = array![
            [0.2, 0.5, 0.0, 0.0],
            [0.0, 3.0, -0.4, 0.0],
            [0.0, 0.0, 1.7, 0.0],
            [0.0, 0.0, 0.0, 2.5]
        ];
        let primary_t = fast_atb(&transform, &fast_ab(&embedded, &transform));
        let gram_t = matern_center_function_gram(&embedded, true, Some(&transform))
            .expect("transformed center function Gram");
        let transformed = matern_double_penalty_candidates(&primary_t, &gram_t, true)
            .expect("transformed candidates");
        let ridge_t = transformed[1].matrix.dense() * transformed[1].normalization_scale;
        let expected = fast_atb(&transform, &fast_ab(&raw_ridge, &transform));
        let covariance_error = (&ridge_t - &expected)
            .iter()
            .map(|value| value.abs())
            .fold(0.0_f64, f64::max);
        assert!(
            covariance_error < 2.0e-12,
            "Matérn function ridge changed under a basis chart; error={covariance_error:.3e}"
        );

        let no_intercept_gram = matern_center_function_gram(
            &center_kernel,
            false,
            Some(&transform.slice(s![0..3, 0..3]).to_owned()),
        )
        .expect("kernel-only Gram");
        let kernel_only = matern_double_penalty_candidates(
            &fast_atb(
                &transform.slice(s![0..3, 0..3]).to_owned(),
                &fast_ab(&center_kernel, &transform.slice(s![0..3, 0..3]).to_owned()),
            ),
            &no_intercept_gram,
            false,
        )
        .expect("kernel-only candidates");
        assert_eq!(kernel_only.len(), 1, "an SPD kernel has no null ridge");
    }
}

/// Auto-derive a streaming row chunk size for dense basis evaluation.
///
/// The opt-in `streaming_chunk_size` knob has been removed from public specs:
/// streaming activates automatically when the would-be dense buffer
/// `n_rows * n_basis_cols * 8 bytes` exceeds 1 GiB. When streaming is
/// active, the chunk size is sized so each resident chunk holds ~256 MiB
/// of `f64` (`chunk = (256 MiB) / (n_basis_cols * 8)`), clamped to
/// `[1024, n_rows]`. Returning `None` means "do not stream, materialize
/// densely".
pub fn auto_streaming_chunk_size_for_dense(n_rows: usize, n_basis_cols: usize) -> Option<usize> {
    if n_rows == 0 || n_basis_cols == 0 {
        return None;
    }
    const DENSE_THRESHOLD_BYTES: usize = 1024 * 1024 * 1024;
    const TARGET_CHUNK_BYTES: usize = 256 * 1024 * 1024;
    const MIN_CHUNK_ROWS: usize = 1024;
    let dense_bytes = n_rows.saturating_mul(n_basis_cols).saturating_mul(8);
    if dense_bytes <= DENSE_THRESHOLD_BYTES {
        return None;
    }
    let row_bytes = n_basis_cols.saturating_mul(8).max(1);
    let raw_chunk = TARGET_CHUNK_BYTES / row_bytes;
    let clamped = raw_chunk.max(MIN_CHUNK_ROWS).min(n_rows);
    Some(clamped)
}