gam_model_kernels/

cubic_cell_kernel.rs

use gam_math::probability::normal_cdf;
use gam_runtime::resource::{ByteLruCache, ResidentBytes};
use smallvec::{SmallVec, smallvec};
use std::hash::{Hash, Hasher};
use std::sync::Arc;
use std::sync::atomic::{AtomicU64, Ordering};

/// Typed errors raised by the de-nested cubic transport kernel.
///
/// Sibling families (`bernoulli_marginal_slope`, `survival_marginal_slope`,
/// `marginal_slope_shared`) currently consume the kernel's public surface via
/// `Result<_, String>`. To stay source-compatible, the kernel converts errors
/// to `String` at the boundary via `From<CubicCellKernelError> for String` and
/// keeps the public function signatures returning `Result<_, String>`.
/// `Display` is exact-byte-equivalent to the previous `format!(...)` strings.
#[derive(Clone, Debug)]
pub enum CubicCellKernelError {
    /// Interval probe / cell-bounds preconditions (ordered bounds, supported
    /// infinity patterns, positive finite width).
    InvalidInterval { reason: String },
    /// Cell-shape / branch-classification failure: tail cells not affine,
    /// finite cells with non-positive width, non-finite affine coefficients,
    /// non-affine cell with infinite bounds, leading-coefficient degeneracy
    /// in the moment recurrence, etc.
    InvalidCellShape { reason: String },
    /// Reduced moment vector (or polynomial-convolution scratch) is shorter
    /// than the polynomial degree the leaf needs to evaluate.
    InsufficientMoments { reason: String },
    /// Bivariate-normal CDF domain validation (non-finite/non-infinite
    /// argument, non-finite correlation).
    BivariateNormalDomain { reason: String },
}

impl_reason_error_boilerplate! {
    CubicCellKernelError {
        InvalidInterval,
        InvalidCellShape,
        InsufficientMoments,
        BivariateNormalDomain,
    }
}

impl CubicCellKernelError {
    #[inline]
    fn invalid_interval(reason: impl Into<String>) -> Self {
        CubicCellKernelError::InvalidInterval {
            reason: reason.into(),
        }
    }
    #[inline]
    fn invalid_cell_shape(reason: impl Into<String>) -> Self {
        CubicCellKernelError::InvalidCellShape {
            reason: reason.into(),
        }
    }
    #[inline]
    fn insufficient_moments(reason: impl Into<String>) -> Self {
        CubicCellKernelError::InsufficientMoments {
            reason: reason.into(),
        }
    }
    #[inline]
    fn bivariate_normal_domain(reason: impl Into<String>) -> Self {
        CubicCellKernelError::BivariateNormalDomain {
            reason: reason.into(),
        }
    }
}

// De-nested cubic transport kernel.
//
// This module implements the de-nested flexible-link/score-warp model
//
//   eta(z) = a + b*z + b*delta_h(z) + delta_w(a + b*z)
//
// where delta_h is the score warp and delta_w is the link deviation.
// This is not the literal nested composition L(a + b*H(z)); it is an
// additive-correction model around the affine core a + b*z.
//
// On each partition cell, both deviations are cubic polynomials, so eta is
// at most sextic in z and q(z) = 0.5*(z^2 + eta^2) is at most degree 12.
// The integral of exp(-q(z)) is evaluated by transporting from the affine
// anchor (c2=c3=0, where q is Gaussian and the integral reduces to BVN)
// to the target non-affine cell via the polynomial moment recurrence.
//
// The partition covers (-∞, +∞) with:
//   • two semi-infinite affine TAIL cells (outside all deviation support),
//   • finitely many interior cells (each a sextic microcell).
// Because tail cells have constant deviations (c2=c3=0), their bounds
// are parameter-independent, so no Leibniz boundary-motion corrections
// appear in the derivatives.
//
// Shared by bernoulli_marginal_slope and survival_marginal_slope families.

#[derive(Clone, Copy, Debug, PartialEq)]
pub struct LocalSpanCubic {
    pub left: f64,
    pub right: f64,
    pub c0: f64,
    pub c1: f64,
    pub c2: f64,
    pub c3: f64,
}

impl LocalSpanCubic {
    #[inline]
    pub fn evaluate(self, x: f64) -> f64 {
        let t = x - self.left;
        self.c0 + self.c1 * t + self.c2 * t * t + self.c3 * t * t * t
    }

    #[inline]
    pub fn first_derivative(self, x: f64) -> f64 {
        let t = x - self.left;
        self.c1 + 2.0 * self.c2 * t + 3.0 * self.c3 * t * t
    }

    #[inline]
    pub fn second_derivative(self, x: f64) -> f64 {
        let t = x - self.left;
        2.0 * self.c2 + 6.0 * self.c3 * t
    }
}

pub const ANCHORED_DEVIATION_KERNEL: &str = "DenestedCubicTransport";
/// Default normalized non-affine branch tolerance used by [`branch_cell`].
///
/// Keep this cutoff explicit and hill-climbable: the large-scale cycle-0
/// sweep evaluated `{1e-12, 1e-10, 1e-8, 1e-6, 1e-4, 1e-3}` against the
/// legacy transport path.  The more aggressive candidates require an
/// end-to-end beta acceptance run before promotion; the default therefore
/// remains the legacy `1e-10` value to preserve bit-for-bit model behavior.
pub const NORMALIZED_CELL_BRANCH_TOL: f64 = 1e-10;

const INV_TWO_PI: f64 = 1.0 / std::f64::consts::TAU;

/// 384-point Gauss–Legendre nodes, re-exported for the GPU cubic-cell kernel
/// (`src/gpu/cubic_cell/kernel_src.rs`) to embed as `__constant__` device
/// memory. Linux-only because the kernel emitter is Linux-only.
#[cfg(target_os = "linux")]
pub const GL_NODES_FOR_GPU_KERNEL: &[f64; 384] = &GL_NODES;
/// Companion weights to [`GL_NODES_FOR_GPU_KERNEL`].
#[cfg(target_os = "linux")]
pub const GL_WEIGHTS_FOR_GPU_KERNEL: &[f64; 384] = &GL_WEIGHTS;

const GL_NODES: [f64; 384] = [
    -9.999_804_411_726_474e-1,
    -9.998_969_471_378_596e-1,
    -9.997_467_408_113_523e-1,
    -9.995_297_988_558_859e-1,
    -9.992_461_316_671_845e-1,
    -9.988_957_572_063_257e-1,
    -9.984_786_985_384_589e-1,
    -9.979_949_833_727_938e-1,
    -9.974_446_439_389_107e-1,
    -9.968_277_169_440_913e-1,
    -9.961_442_435_551_087e-1,
    -9.953_942_693_885_953e-1,
    -9.945_778_445_047_068e-1,
    -9.936_950_234_020_883e-1,
    -9.927_458_650_133_153e-1,
    -9.917_304_327_004_32e-1,
    -9.906_487_942_504_061e-1,
    -9.895_010_218_704_087e-1,
    -9.882_871_921_828_699e-1,
    -9.870_073_862_202_815e-1,
    -9.856_616_894_197_333e-1,
    -9.842_501_916_171_713e-1,
    -9.827_729_870_413_743e-1,
    -9.812_301_743_076_443e-1,
    -9.796_218_564_112_101e-1,
    -9.779_481_407_203_411e-1,
    -9.762_091_389_691_724e-1,
    -9.744_049_672_502_397e-1,
    -9.725_357_460_067_257e-1,
    -9.706_016_000_244_151e-1,
    -9.686_026_584_233_628e-1,
    -9.665_390_546_492_71e-1,
    -9.644_109_264_645_802e-1,
    -9.622_184_159_392_698e-1,
    -9.599_616_694_413_742e-1,
    -9.576_408_376_272_095e-1,
    -9.552_560_754_313_16e-1,
    -9.528_075_420_561_144e-1,
    -9.502_954_009_612_771e-1,
    -9.477_198_198_528_157e-1,
    -9.450_809_706_718_851e-1,
    -9.423_790_295_833_044e-1,
    -9.396_141_769_637_963e-1,
    -9.367_865_973_899_459e-1,
    -9.338_964_796_258_775e-1,
    -9.309_440_166_106_54e-1,
    -9.279_294_054_453_956e-1,
    -9.248_528_473_801_222e-1,
    -9.217_145_478_003_181e-1,
    -9.185_147_162_132_208e-1,
    -9.152_535_662_338_34e-1,
    -9.119_313_155_706_682e-1,
    -9.085_481_860_112_055e-1,
    -9.051_044_034_070_944e-1,
    -9.016_001_976_590_722e-1,
    -8.980_358_027_016_164e-1,
    -8.944_114_564_873_288e-1,
    -8.907_274_009_710_492e-1,
    -8.869_838_820_937_034e-1,
    -8.831_811_497_658_847e-1,
    -8.793_194_578_511_7e-1,
    -8.753_990_641_491_725e-1,
    -8.714_202_303_783_312e-1,
    -8.673_832_221_584_393e-1,
    -8.632_883_089_929_12e-1,
    -8.591_357_642_507_945e-1,
    -8.549_258_651_485_127e-1,
    -8.506_588_927_313_666e-1,
    -8.463_351_318_547_683e-1,
    -8.419_548_711_652_254e-1,
    -8.375_184_030_810_715e-1,
    -8.330_260_237_729_452e-1,
    -8.284_780_331_440_178e-1,
    -8.238_747_348_099_726e-1,
    -8.192_164_360_787_36e-1,
    -8.145_034_479_299_62e-1,
    -8.097_360_849_942_72e-1,
    -8.049_146_655_322_506e-1,
    -8.000_395_114_131_988e-1,
    -7.951_109_480_936_471e-1,
    -7.901_293_045_956_28e-1,
    -7.850_949_134_847_117e-1,
    -7.800_081_108_478_04e-1,
    -7.748_692_362_707_1e-1,
    -7.696_786_328_154_644e-1,
    -7.644_366_469_974_285e-1,
    -7.591_436_287_621_58e-1,
    -7.537_999_314_620_412e-1,
    -7.484_059_118_327_094e-1,
    -7.429_619_299_692_227e-1,
    -7.374_683_493_020_299e-1,
    -7.319_255_365_727_068e-1,
    -7.263_338_618_094_733e-1,
    -7.206_936_983_024_912e-1,
    -7.150_054_225_789_432e-1,
    -7.092_694_143_778_975e-1,
    -7.034_860_566_249_567e-1,
    -6.976_557_354_066_943e-1,
    -6.917_788_399_448_808e-1,
    -6.858_557_625_704_99e-1,
    -6.798_868_986_975_534e-1,
    -6.738_726_467_966_731e-1,
    -6.678_134_083_685_102e-1,
    -6.617_095_879_169_366e-1,
    -6.555_615_929_220_4e-1,
    -6.493_698_338_129_212e-1,
    -6.431_347_239_402_948e-1,
    -6.368_566_795_488_945e-1,
    -6.305_361_197_496_849e-1,
    -6.241_734_664_918_837e-1,
    -6.177_691_445_347_913e-1,
    -6.113_235_814_194_364e-1,
    -6.048_372_074_400_329e-1,
    -5.983_104_556_152_549e-1,
    -5.917_437_616_593_286e-1,
    -5.851_375_639_529_456e-1,
    -5.784_923_035_139_965e-1,
    -5.718_084_239_681_3e-1,
    -5.650_863_715_191_369e-1,
    -5.583_265_949_191_623e-1,
    -5.515_295_454_387_482e-1,
    -5.446_956_768_367_068e-1,
    -5.378_254_453_298_289e-1,
    -5.309_193_095_624_275e-1,
    -5.239_777_305_757_194e-1,
    -5.170_011_717_770_473e-1,
    -5.099_900_989_089_429e-1,
    -5.029_449_800_180_356e-1,
    -4.958_662_854_238_058_4e-1,
    -4.887_544_876_871_878e-1,
    -4.816_100_615_790_221e-1,
    -4.744_334_840_483_605_5e-1,
    -4.672_252_341_906_264e-1,
    -4.599_857_932_156_304e-1,
    -4.527_156_444_154_463_7e-1,
    -4.454_152_731_321_473_5e-1,
    -4.380_851_667_254_05e-1,
    -4.307_258_145_399_544_5e-1,
    -4.233_377_078_729_265e-1,
    -4.159_213_399_410_494e-1,
    -4.084_772_058_477_228e-1,
    -4.010_058_025_499_653e-1,
    -3.935_076_288_252_386e-1,
    -3.859_831_852_381_500_6e-1,
    -3.784_329_741_070_358_6e-1,
    -3.708_574_994_704_271e-1,
    -3.632_572_670_534_011e-1,
    -3.556_327_842_338_202e-1,
    -3.479_845_600_084_600_6e-1,
    -3.403_131_049_590_297e-1,
    -3.326_189_312_180_866e-1,
    -3.249_025_524_348_469_5e-1,
    -3.171_644_837_408_958_4e-1,
    -3.094_052_417_157_978e-1,
    -3.016_253_443_526_109e-1,
    -2.938_253_110_233_064_5e-1,
    -2.860_056_624_440_967_5e-1,
    -2.781_669_206_406_729e-1,
    -2.703_096_089_133_553e-1,
    -2.624_342_518_021_592_4e-1,
    -2.545_413_750_517_773e-1,
    -2.466_315_055_764_817_5e-1,
    -2.387_051_714_249_486_3e-1,
    -2.307_629_017_450_062e-1,
    -2.228_052_267_483_099_4e-1,
    -2.148_326_776_749_466_5e-1,
    -2.068_457_867_579_697_5e-1,
    -1.988_450_871_878_683_4e-1,
    -1.908_311_130_769_724_5e-1,
    -1.828_043_994_237_965_6e-1,
    -1.747_654_820_773_241_2e-1,
    -1.667_148_977_012_352_4e-1,
    -1.586_531_837_380_799_3e-1,
    -1.505_808_783_733_995e-1,
    -1.424_985_204_997_981_4e-1,
    -1.344_066_496_809_674_7e-1,
    -1.263_058_061_156_663e-1,
    -1.181_965_306_016_578_4e-1,
    -1.100_793_644_996_070_4e-1,
    -1.019_548_496_969_403_7e-1,
    -9.382_352_857_167_028e-2,
    -8.568_594_395_618_719e-2,
    -7.754_263_910_102_077e-2,
    -6.939_415_763_857_37e-2,
    -6.124_104_354_682_962e-2,
    -5.308_384_111_303_817_6e-2,
    -4.492_309_489_737_94e-2,
    -3.675_934_969_660_982e-2,
    -2.859_315_050_769_284_7e-2,
    -2.042_504_249_141_571e-2,
    -1.225_557_093_599_553_8e-2,
    -4.085_281_220_676_868e-3,
    4.085_281_220_676_868e-3,
    1.225_557_093_599_553_8e-2,
    2.042_504_249_141_571e-2,
    2.859_315_050_769_284_7e-2,
    3.675_934_969_660_982e-2,
    4.492_309_489_737_94e-2,
    5.308_384_111_303_817_6e-2,
    6.124_104_354_682_962e-2,
    6.939_415_763_857_37e-2,
    7.754_263_910_102_077e-2,
    8.568_594_395_618_719e-2,
    9.382_352_857_167_028e-2,
    1.019_548_496_969_403_7e-1,
    1.100_793_644_996_070_4e-1,
    1.181_965_306_016_578_4e-1,
    1.263_058_061_156_663e-1,
    1.344_066_496_809_674_7e-1,
    1.424_985_204_997_981_4e-1,
    1.505_808_783_733_995e-1,
    1.586_531_837_380_799_3e-1,
    1.667_148_977_012_352_4e-1,
    1.747_654_820_773_241_2e-1,
    1.828_043_994_237_965_6e-1,
    1.908_311_130_769_724_5e-1,
    1.988_450_871_878_683_4e-1,
    2.068_457_867_579_697_5e-1,
    2.148_326_776_749_466_5e-1,
    2.228_052_267_483_099_4e-1,
    2.307_629_017_450_062e-1,
    2.387_051_714_249_486_3e-1,
    2.466_315_055_764_817_5e-1,
    2.545_413_750_517_773e-1,
    2.624_342_518_021_592_4e-1,
    2.703_096_089_133_553e-1,
    2.781_669_206_406_729e-1,
    2.860_056_624_440_967_5e-1,
    2.938_253_110_233_064_5e-1,
    3.016_253_443_526_109e-1,
    3.094_052_417_157_978e-1,
    3.171_644_837_408_958_4e-1,
    3.249_025_524_348_469_5e-1,
    3.326_189_312_180_866e-1,
    3.403_131_049_590_297e-1,
    3.479_845_600_084_600_6e-1,
    3.556_327_842_338_202e-1,
    3.632_572_670_534_011e-1,
    3.708_574_994_704_271e-1,
    3.784_329_741_070_358_6e-1,
    3.859_831_852_381_500_6e-1,
    3.935_076_288_252_386e-1,
    4.010_058_025_499_653e-1,
    4.084_772_058_477_228e-1,
    4.159_213_399_410_494e-1,
    4.233_377_078_729_265e-1,
    4.307_258_145_399_544_5e-1,
    4.380_851_667_254_05e-1,
    4.454_152_731_321_473_5e-1,
    4.527_156_444_154_463_7e-1,
    4.599_857_932_156_304e-1,
    4.672_252_341_906_264e-1,
    4.744_334_840_483_605_5e-1,
    4.816_100_615_790_221e-1,
    4.887_544_876_871_878e-1,
    4.958_662_854_238_058_4e-1,
    5.029_449_800_180_356e-1,
    5.099_900_989_089_429e-1,
    5.170_011_717_770_473e-1,
    5.239_777_305_757_194e-1,
    5.309_193_095_624_275e-1,
    5.378_254_453_298_289e-1,
    5.446_956_768_367_068e-1,
    5.515_295_454_387_482e-1,
    5.583_265_949_191_623e-1,
    5.650_863_715_191_369e-1,
    5.718_084_239_681_3e-1,
    5.784_923_035_139_965e-1,
    5.851_375_639_529_456e-1,
    5.917_437_616_593_286e-1,
    5.983_104_556_152_549e-1,
    6.048_372_074_400_329e-1,
    6.113_235_814_194_364e-1,
    6.177_691_445_347_913e-1,
    6.241_734_664_918_837e-1,
    6.305_361_197_496_849e-1,
    6.368_566_795_488_945e-1,
    6.431_347_239_402_948e-1,
    6.493_698_338_129_212e-1,
    6.555_615_929_220_4e-1,
    6.617_095_879_169_366e-1,
    6.678_134_083_685_102e-1,
    6.738_726_467_966_731e-1,
    6.798_868_986_975_534e-1,
    6.858_557_625_704_99e-1,
    6.917_788_399_448_808e-1,
    6.976_557_354_066_943e-1,
    7.034_860_566_249_567e-1,
    7.092_694_143_778_975e-1,
    7.150_054_225_789_432e-1,
    7.206_936_983_024_912e-1,
    7.263_338_618_094_733e-1,
    7.319_255_365_727_068e-1,
    7.374_683_493_020_299e-1,
    7.429_619_299_692_227e-1,
    7.484_059_118_327_094e-1,
    7.537_999_314_620_412e-1,
    7.591_436_287_621_58e-1,
    7.644_366_469_974_285e-1,
    7.696_786_328_154_644e-1,
    7.748_692_362_707_1e-1,
    7.800_081_108_478_04e-1,
    7.850_949_134_847_117e-1,
    7.901_293_045_956_28e-1,
    7.951_109_480_936_471e-1,
    8.000_395_114_131_988e-1,
    8.049_146_655_322_506e-1,
    8.097_360_849_942_72e-1,
    8.145_034_479_299_62e-1,
    8.192_164_360_787_36e-1,
    8.238_747_348_099_726e-1,
    8.284_780_331_440_178e-1,
    8.330_260_237_729_452e-1,
    8.375_184_030_810_715e-1,
    8.419_548_711_652_254e-1,
    8.463_351_318_547_683e-1,
    8.506_588_927_313_666e-1,
    8.549_258_651_485_127e-1,
    8.591_357_642_507_945e-1,
    8.632_883_089_929_12e-1,
    8.673_832_221_584_393e-1,
    8.714_202_303_783_312e-1,
    8.753_990_641_491_725e-1,
    8.793_194_578_511_7e-1,
    8.831_811_497_658_847e-1,
    8.869_838_820_937_034e-1,
    8.907_274_009_710_492e-1,
    8.944_114_564_873_288e-1,
    8.980_358_027_016_164e-1,
    9.016_001_976_590_722e-1,
    9.051_044_034_070_944e-1,
    9.085_481_860_112_055e-1,
    9.119_313_155_706_682e-1,
    9.152_535_662_338_34e-1,
    9.185_147_162_132_208e-1,
    9.217_145_478_003_181e-1,
    9.248_528_473_801_222e-1,
    9.279_294_054_453_956e-1,
    9.309_440_166_106_54e-1,
    9.338_964_796_258_775e-1,
    9.367_865_973_899_459e-1,
    9.396_141_769_637_963e-1,
    9.423_790_295_833_044e-1,
    9.450_809_706_718_851e-1,
    9.477_198_198_528_157e-1,
    9.502_954_009_612_771e-1,
    9.528_075_420_561_144e-1,
    9.552_560_754_313_16e-1,
    9.576_408_376_272_095e-1,
    9.599_616_694_413_742e-1,
    9.622_184_159_392_698e-1,
    9.644_109_264_645_802e-1,
    9.665_390_546_492_71e-1,
    9.686_026_584_233_628e-1,
    9.706_016_000_244_151e-1,
    9.725_357_460_067_257e-1,
    9.744_049_672_502_397e-1,
    9.762_091_389_691_724e-1,
    9.779_481_407_203_411e-1,
    9.796_218_564_112_101e-1,
    9.812_301_743_076_443e-1,
    9.827_729_870_413_743e-1,
    9.842_501_916_171_713e-1,
    9.856_616_894_197_333e-1,
    9.870_073_862_202_815e-1,
    9.882_871_921_828_699e-1,
    9.895_010_218_704_087e-1,
    9.906_487_942_504_061e-1,
    9.917_304_327_004_32e-1,
    9.927_458_650_133_153e-1,
    9.936_950_234_020_883e-1,
    9.945_778_445_047_068e-1,
    9.953_942_693_885_953e-1,
    9.961_442_435_551_087e-1,
    9.968_277_169_440_913e-1,
    9.974_446_439_389_107e-1,
    9.979_949_833_727_938e-1,
    9.984_786_985_384_589e-1,
    9.988_957_572_063_257e-1,
    9.992_461_316_671_845e-1,
    9.995_297_988_558_859e-1,
    9.997_467_408_113_523e-1,
    9.998_969_471_378_596e-1,
    9.999_804_411_726_474e-1,
];
const GL_WEIGHTS: [f64; 384] = [
    5.019_410_348_676_869_6e-5,
    1.168_390_665_730_266_3e-4,
    1.835_749_193_551_655_8e-4,
    2.503_070_890_844_105e-4,
    3.170_242_698_112_815e-4,
    3.837_208_020_912_921_4e-4,
    4.503_919_137_716_827e-4,
    5.170_330_453_491_649e-4,
    5.836_397_042_630_135e-4,
    6.502_074_240_969_948e-4,
    7.167_317_509_947_801e-4,
    7.832_082_385_905_168e-4,
    8.496_324_460_039_209e-4,
    9.159_999_370_632_641e-4,
    9.823_062_800_663_463e-4,
    1.048_547_047_793_689_5e-3,
    1.114_717_817_647_310_6e-3,
    1.180_814_171_855_922e-3,
    1.246_831_697_715_441_5e-3,
    1.312_765_987_850_66e-3,
    1.378_612_640_487_646_8e-3,
    1.444_367_259_734_736e-3,
    1.510_025_455_865_810_3e-3,
    1.575_582_845_607_936_8e-3,
    1.641_035_052_429_271_5e-3,
    1.706_377_706_828_447_1e-3,
    1.771_606_446_623_834_7e-3,
    1.836_716_917_243_567_5e-3,
    1.901_704_772_014_899_2e-3,
    1.966_565_672_453_437e-3,
    2.031_295_288_552_398_4e-3,
    2.095_889_299_071_020_6e-3,
    2.160_343_391_822_734_3e-3,
    2.224_653_263_962_713e-3,
    2.288_814_622_274_955e-3,
    2.352_823_183_458_769e-3,
    2.416_674_674_414_340_5e-3,
    2.480_364_832_528_265_6e-3,
    2.543_889_405_957_74e-3,
    2.607_244_153_914_452e-3,
    2.670_424_846_947_554e-3,
    2.733_427_267_226_093_3e-3,
    2.796_247_208_820_428e-3,
    2.858_880_477_983_06e-3,
    2.921_322_893_428_515_3e-3,
    2.983_570_286_612_554_5e-3,
    3.045_618_502_010_327_8e-3,
    3.107_463_397_393_755_5e-3,
    3.169_100_844_108_32e-3,
    3.230_526_727_348_174e-3,
    3.291_736_946_431_361e-3,
    3.352_727_415_073_250_3e-3,
    3.413_494_061_659_418_4e-3,
    3.474_032_829_517_317e-3,
    3.534_339_677_187_348_4e-3,
    3.594_410_578_692_452e-3,
    3.654_241_523_806_987e-3,
    3.713_828_518_324_312_5e-3,
    3.773_167_584_323_583_5e-3,
    3.832_254_760_435_171e-3,
    3.891_086_102_105_193_4e-3,
    3.949_657_681_858_895e-3,
    4.007_965_589_562_678e-3,
    4.066_005_932_685_269e-3,
    4.123_774_836_557_6e-3,
    4.181_268_444_631_281e-3,
    4.238_482_918_736_289e-3,
    4.295_414_439_336_925e-3,
    4.352_059_205_787_275e-3,
    4.408_413_436_584_285e-3,
    4.464_473_369_620_78e-3,
    4.520_235_262_436_235e-3,
    4.575_695_392_466_791e-3,
    4.630_850_057_293_894e-3,
    4.685_695_574_891_041e-3,
    4.740_228_283_870_022e-3,
    4.794_444_543_725_102e-3,
    4.848_340_735_076_109e-3,
    4.901_913_259_910_197e-3,
    4.955_158_541_821_682_4e-3,
    5.008_073_026_251_332e-3,
    5.060_653_180_723_101_4e-3,
    5.112_895_495_080_397e-3,
    5.164_796_481_720_011e-3,
    5.216_352_675_825_451e-3,
    5.267_560_635_597_735e-3,
    5.318_416_942_485_385e-3,
    5.368_918_201_412_827e-3,
    5.419_061_041_006_627e-3,
    5.468_842_113_820_941e-3,
    5.518_258_096_560_71e-3,
    5.567_305_690_303_767e-3,
    5.615_981_620_720_803e-3,
    5.664_282_638_294_182e-3,
    5.712_205_518_534_655e-3,
    5.759_747_062_196_925_5e-3,
    5.806_904_095_492_818e-3,
    5.853_673_470_303_617_4e-3,
    5.900_052_064_389_824e-3,
    5.946_036_781_599_814e-3,
    5.991_624_552_076_468e-3,
    6.036_812_332_462_087e-3,
    6.081_597_106_101_673e-3,
    6.125_975_883_244_196e-3,
    6.169_945_701_242_237e-3,
    6.213_503_624_749_591e-3,
    6.256_646_745_917_723e-3,
    6.299_372_184_589_237e-3,
    6.341_677_088_490_664e-3,
    6.383_558_633_422_572e-3,
    6.425_014_023_448_273e-3,
    6.466_040_491_080_434e-3,
    6.506_635_297_465_724e-3,
    6.546_795_732_567_842_5e-3,
    6.586_519_115_348_261e-3,
    6.625_802_793_945_317e-3,
    6.664_644_145_851_14e-3,
    6.703_040_578_086_941e-3,
    6.740_989_527_375_895e-3,
    6.778_488_460_314_126e-3,
    6.815_534_873_540_5e-3,
    6.852_126_293_902_878e-3,
    6.888_260_278_623_754e-3,
    6.923_934_415_463_31e-3,
    6.959_146_322_880_146_5e-3,
    6.993_893_650_190_702e-3,
    7.028_174_077_725_734e-3,
    7.061_985_316_985_506e-3,
    7.095_325_110_792_439e-3,
    7.128_191_233_441_844e-3,
    7.160_581_490_850_321e-3,
    7.192_493_720_702_486e-3,
    7.223_925_792_595_309e-3,
    7.254_875_608_179_984e-3,
    7.285_341_101_302_512e-3,
    7.315_320_238_141_324_5e-3,
    7.344_811_017_343_063e-3,
    7.373_811_470_156_258e-3,
    7.402_319_660_562_818e-3,
    7.430_333_685_407_178e-3,
    7.457_851_674_523_319e-3,
    7.484_871_790_859_79e-3,
    7.511_392_230_602_079e-3,
    7.537_411_223_293_362e-3,
    7.562_927_031_952_382e-3,
    7.587_937_953_189_561_5e-3,
    7.612_442_317_320_796e-3,
    7.636_438_488_478_739e-3,
    7.659_924_864_722_064e-3,
    7.682_899_878_142_539e-3,
    7.705_361_994_969_524e-3,
    7.727_309_715_672_44e-3,
    7.748_741_575_060_914e-3,
    7.769_656_142_382_462e-3,
    7.790_052_021_418_226e-3,
    7.809_927_850_575_903e-3,
    7.829_282_302_980_82e-3,
    7.848_114_086_564_56e-3,
    7.866_421_944_151_094e-3,
    7.884_204_653_540_665e-3,
    7.901_461_027_591_6e-3,
    7.918_189_914_299_318e-3,
    7.934_390_196_873_448e-3,
    7.950_060_793_812_204e-3,
    7.965_200_658_974_709e-3,
    7.979_808_781_650_77e-3,
    7.993_884_186_628_266e-3,
    8.007_425_934_258_548e-3,
    8.020_433_120_518_866e-3,
    8.032_904_877_072_8e-3,
    8.044_840_371_328_26e-3,
    8.056_238_806_493_175e-3,
    8.067_099_421_628_42e-3,
    8.077_421_491_698_82e-3,
    8.087_204_327_621_594e-3,
    8.096_447_276_312_202e-3,
    8.105_149_720_727_933e-3,
    8.113_311_079_909_208e-3,
    8.120_930_809_018_415e-3,
    8.128_008_399_376_085e-3,
    8.134_543_378_495_033e-3,
    8.140_535_310_111_77e-3,
    8.145_983_794_215_77e-3,
    8.150_888_467_075_875e-3,
    8.155_249_001_265_092e-3,
    8.159_065_105_681_899e-3,
    8.162_336_525_570_1e-3,
    8.165_063_042_535_465e-3,
    8.167_244_474_560_707e-3,
    8.168_880_676_017_344e-3,
    8.169_971_537_675_47e-3,
    8.170_516_986_711_104e-3,
    8.170_516_986_711_104e-3,
    8.169_971_537_675_47e-3,
    8.168_880_676_017_344e-3,
    8.167_244_474_560_707e-3,
    8.165_063_042_535_465e-3,
    8.162_336_525_570_1e-3,
    8.159_065_105_681_899e-3,
    8.155_249_001_265_092e-3,
    8.150_888_467_075_875e-3,
    8.145_983_794_215_77e-3,
    8.140_535_310_111_77e-3,
    8.134_543_378_495_033e-3,
    8.128_008_399_376_085e-3,
    8.120_930_809_018_415e-3,
    8.113_311_079_909_208e-3,
    8.105_149_720_727_933e-3,
    8.096_447_276_312_202e-3,
    8.087_204_327_621_594e-3,
    8.077_421_491_698_82e-3,
    8.067_099_421_628_42e-3,
    8.056_238_806_493_175e-3,
    8.044_840_371_328_26e-3,
    8.032_904_877_072_8e-3,
    8.020_433_120_518_866e-3,
    8.007_425_934_258_548e-3,
    7.993_884_186_628_266e-3,
    7.979_808_781_650_77e-3,
    7.965_200_658_974_709e-3,
    7.950_060_793_812_204e-3,
    7.934_390_196_873_448e-3,
    7.918_189_914_299_318e-3,
    7.901_461_027_591_6e-3,
    7.884_204_653_540_665e-3,
    7.866_421_944_151_094e-3,
    7.848_114_086_564_56e-3,
    7.829_282_302_980_82e-3,
    7.809_927_850_575_903e-3,
    7.790_052_021_418_226e-3,
    7.769_656_142_382_462e-3,
    7.748_741_575_060_914e-3,
    7.727_309_715_672_44e-3,
    7.705_361_994_969_524e-3,
    7.682_899_878_142_539e-3,
    7.659_924_864_722_064e-3,
    7.636_438_488_478_739e-3,
    7.612_442_317_320_796e-3,
    7.587_937_953_189_561_5e-3,
    7.562_927_031_952_382e-3,
    7.537_411_223_293_362e-3,
    7.511_392_230_602_079e-3,
    7.484_871_790_859_79e-3,
    7.457_851_674_523_319e-3,
    7.430_333_685_407_178e-3,
    7.402_319_660_562_818e-3,
    7.373_811_470_156_258e-3,
    7.344_811_017_343_063e-3,
    7.315_320_238_141_324_5e-3,
    7.285_341_101_302_512e-3,
    7.254_875_608_179_984e-3,
    7.223_925_792_595_309e-3,
    7.192_493_720_702_486e-3,
    7.160_581_490_850_321e-3,
    7.128_191_233_441_844e-3,
    7.095_325_110_792_439e-3,
    7.061_985_316_985_506e-3,
    7.028_174_077_725_734e-3,
    6.993_893_650_190_702e-3,
    6.959_146_322_880_146_5e-3,
    6.923_934_415_463_31e-3,
    6.888_260_278_623_754e-3,
    6.852_126_293_902_878e-3,
    6.815_534_873_540_5e-3,
    6.778_488_460_314_126e-3,
    6.740_989_527_375_895e-3,
    6.703_040_578_086_941e-3,
    6.664_644_145_851_14e-3,
    6.625_802_793_945_317e-3,
    6.586_519_115_348_261e-3,
    6.546_795_732_567_842_5e-3,
    6.506_635_297_465_724e-3,
    6.466_040_491_080_434e-3,
    6.425_014_023_448_273e-3,
    6.383_558_633_422_572e-3,
    6.341_677_088_490_664e-3,
    6.299_372_184_589_237e-3,
    6.256_646_745_917_723e-3,
    6.213_503_624_749_591e-3,
    6.169_945_701_242_237e-3,
    6.125_975_883_244_196e-3,
    6.081_597_106_101_673e-3,
    6.036_812_332_462_087e-3,
    5.991_624_552_076_468e-3,
    5.946_036_781_599_814e-3,
    5.900_052_064_389_824e-3,
    5.853_673_470_303_617_4e-3,
    5.806_904_095_492_818e-3,
    5.759_747_062_196_925_5e-3,
    5.712_205_518_534_655e-3,
    5.664_282_638_294_182e-3,
    5.615_981_620_720_803e-3,
    5.567_305_690_303_767e-3,
    5.518_258_096_560_71e-3,
    5.468_842_113_820_941e-3,
    5.419_061_041_006_627e-3,
    5.368_918_201_412_827e-3,
    5.318_416_942_485_385e-3,
    5.267_560_635_597_735e-3,
    5.216_352_675_825_451e-3,
    5.164_796_481_720_011e-3,
    5.112_895_495_080_397e-3,
    5.060_653_180_723_101_4e-3,
    5.008_073_026_251_332e-3,
    4.955_158_541_821_682_4e-3,
    4.901_913_259_910_197e-3,
    4.848_340_735_076_109e-3,
    4.794_444_543_725_102e-3,
    4.740_228_283_870_022e-3,
    4.685_695_574_891_041e-3,
    4.630_850_057_293_894e-3,
    4.575_695_392_466_791e-3,
    4.520_235_262_436_235e-3,
    4.464_473_369_620_78e-3,
    4.408_413_436_584_285e-3,
    4.352_059_205_787_275e-3,
    4.295_414_439_336_925e-3,
    4.238_482_918_736_289e-3,
    4.181_268_444_631_281e-3,
    4.123_774_836_557_6e-3,
    4.066_005_932_685_269e-3,
    4.007_965_589_562_678e-3,
    3.949_657_681_858_895e-3,
    3.891_086_102_105_193_4e-3,
    3.832_254_760_435_171e-3,
    3.773_167_584_323_583_5e-3,
    3.713_828_518_324_312_5e-3,
    3.654_241_523_806_987e-3,
    3.594_410_578_692_452e-3,
    3.534_339_677_187_348_4e-3,
    3.474_032_829_517_317e-3,
    3.413_494_061_659_418_4e-3,
    3.352_727_415_073_250_3e-3,
    3.291_736_946_431_361e-3,
    3.230_526_727_348_174e-3,
    3.169_100_844_108_32e-3,
    3.107_463_397_393_755_5e-3,
    3.045_618_502_010_327_8e-3,
    2.983_570_286_612_554_5e-3,
    2.921_322_893_428_515_3e-3,
    2.858_880_477_983_06e-3,
    2.796_247_208_820_428e-3,
    2.733_427_267_226_093_3e-3,
    2.670_424_846_947_554e-3,
    2.607_244_153_914_452e-3,
    2.543_889_405_957_74e-3,
    2.480_364_832_528_265_6e-3,
    2.416_674_674_414_340_5e-3,
    2.352_823_183_458_769e-3,
    2.288_814_622_274_955e-3,
    2.224_653_263_962_713e-3,
    2.160_343_391_822_734_3e-3,
    2.095_889_299_071_020_6e-3,
    2.031_295_288_552_398_4e-3,
    1.966_565_672_453_437e-3,
    1.901_704_772_014_899_2e-3,
    1.836_716_917_243_567_5e-3,
    1.771_606_446_623_834_7e-3,
    1.706_377_706_828_447_1e-3,
    1.641_035_052_429_271_5e-3,
    1.575_582_845_607_936_8e-3,
    1.510_025_455_865_810_3e-3,
    1.444_367_259_734_736e-3,
    1.378_612_640_487_646_8e-3,
    1.312_765_987_850_66e-3,
    1.246_831_697_715_441_5e-3,
    1.180_814_171_855_922e-3,
    1.114_717_817_647_310_6e-3,
    1.048_547_047_793_689_5e-3,
    9.823_062_800_663_463e-4,
    9.159_999_370_632_641e-4,
    8.496_324_460_039_209e-4,
    7.832_082_385_905_168e-4,
    7.167_317_509_947_801e-4,
    6.502_074_240_969_948e-4,
    5.836_397_042_630_135e-4,
    5.170_330_453_491_649e-4,
    4.503_919_137_716_827e-4,
    3.837_208_020_912_921_4e-4,
    3.170_242_698_112_815e-4,
    2.503_070_890_844_105e-4,
    1.835_749_193_551_655_8e-4,
    1.168_390_665_730_266_3e-4,
    5.019_410_348_676_869_6e-5,
];

#[derive(Clone, Copy, Debug, Eq, PartialEq)]
pub enum ExactCellBranch {
    Affine,
    Quartic,
    Sextic,
}

/// Auto-tune the per-cell affine/non-affine branch tolerance from the cell's
/// own coefficient magnitudes.
///
/// The legacy `branch_cell` compared the normalized cubic coefficients
/// `(k2, k3)` against a single global constant.  That constant is calibrated
/// for cells whose anchor coefficients `(c0, c1)` are O(1).  When the anchor
/// dominates — e.g. a tail cell with `|c0|, |c1| >> 1` — a relative criterion
/// against the anchor magnitude is more numerically meaningful than the bare
/// global threshold, because the affine contribution to `eta` already absorbs
/// any difference at the chosen scale.
///
/// The returned tolerance is always at least [`NORMALIZED_CELL_BRANCH_TOL`],
/// so cells with O(1) anchors recover bit-identical classification with the
/// legacy code path.  This preserves numerical equivalence for the
/// established `cubic_cell_kernel` tests, including the
/// `tuned_branch_tolerance_matches_legacy_non_affine_transport_grid` grid.
#[inline]
fn effective_branch_tol(cell: DenestedCubicCell) -> f64 {
    let anchor_scale = cell.c0.abs().max(cell.c1.abs()).max(1.0);
    NORMALIZED_CELL_BRANCH_TOL * anchor_scale
}

#[derive(Clone, Copy, Debug, PartialEq)]
pub struct DenestedCubicCell {
    pub left: f64,
    pub right: f64,
    pub c0: f64,
    pub c1: f64,
    pub c2: f64,
    pub c3: f64,
}

impl DenestedCubicCell {
    #[inline]
    pub fn eta(self, z: f64) -> f64 {
        self.c0 + self.c1 * z + self.c2 * z * z + self.c3 * z * z * z
    }

    #[inline]
    pub fn q(self, z: f64) -> f64 {
        let eta = self.eta(z);
        0.5 * (z * z + eta * eta)
    }
}

#[derive(Clone, Copy, Debug, Eq, Hash, PartialEq)]
pub struct CellMomentFingerprint {
    pub hash: u64,
    bins: [u64; 6],
}

#[derive(Clone, Copy, Debug, Eq, Hash, PartialEq)]
pub struct CellMomentCacheKey {
    pub fingerprint: CellMomentFingerprint,
    pub max_degree: usize,
}

#[derive(Clone, Copy, Debug, Default, PartialEq)]
pub struct CellMomentDedupStats {
    pub lookups: u64,
    pub hits: u64,
    pub misses: u64,
}

impl CellMomentDedupStats {
    #[inline]
    pub fn hit_rate(self) -> f64 {
        if self.lookups == 0 {
            0.0
        } else {
            self.hits as f64 / self.lookups as f64
        }
    }
}

#[inline]
fn splitmix64(x: u64) -> u64 {
    gam_linalg::utils::splitmix64_hash(x)
}

#[inline]
fn mix_fingerprint_words(words: &[u64]) -> u64 {
    let mut h = 0xcbf2_9ce4_8422_2325u64;
    for &word in words {
        h ^= splitmix64(word);
        h = h.wrapping_mul(0x100_0000_01b3);
    }
    h
}

#[inline]
fn quantized_cell_word(x: f64, epsilon: f64) -> u64 {
    if epsilon == 0.0 || !epsilon.is_finite() || epsilon < 0.0 || !x.is_finite() {
        return x.to_bits();
    }
    (x / epsilon).round().to_bits()
}

/// Returns a deterministic geometric fingerprint for a de-nested cubic cell.
///
/// With `epsilon == 0.0`, each coordinate is represented by its exact IEEE-754
/// bit pattern, so equal fingerprints imply bit-equal `(left, right, c0, c1,
/// c2, c3)` tuples.  With `epsilon > 0`, finite coordinates are binned to the
/// nearest multiple of `epsilon`; callers should treat this as an approximate
/// cache key and validate the resulting model error for their data.
pub fn cell_moment_fingerprint(cell: DenestedCubicCell, epsilon: f64) -> CellMomentFingerprint {
    let bins = [
        quantized_cell_word(cell.left, epsilon),
        quantized_cell_word(cell.right, epsilon),
        quantized_cell_word(cell.c0, epsilon),
        quantized_cell_word(cell.c1, epsilon),
        quantized_cell_word(cell.c2, epsilon),
        quantized_cell_word(cell.c3, epsilon),
    ];
    CellMomentFingerprint {
        hash: mix_fingerprint_words(&bins),
        bins,
    }
}

#[inline]
pub fn cell_moment_cache_key(
    cell: DenestedCubicCell,
    max_degree: usize,
    epsilon: f64,
) -> CellMomentCacheKey {
    CellMomentCacheKey {
        fingerprint: cell_moment_fingerprint(cell, epsilon),
        max_degree,
    }
}

#[derive(Clone, Copy, Debug, PartialEq)]
pub struct DenestedPartitionCell {
    pub cell: DenestedCubicCell,
    pub score_span: LocalSpanCubic,
    pub link_span: LocalSpanCubic,
    /// Provenance of the cell's boundaries: a fixed z location (score break
    /// or ±∞ tail) or a link-knot crossing `z = (τ - a)/b`. Together with
    /// `(score_span, link_span)` this identifies the cell's two-parameter
    /// family in `(a, b)` across rows (see
    /// [`crate::cell_moment_family`]).
    pub left_edge: PartitionEdge,
    pub right_edge: PartitionEdge,
}

impl DenestedPartitionCell {}

/// Provenance of one boundary of a denested partition cell.
#[derive(Clone, Copy, Debug, PartialEq)]
pub enum PartitionEdge {
    /// A z location independent of the row scalars: a score-spline break,
    /// or ±∞ for tail cells.
    Fixed(f64),
    /// A link-knot crossing: the boundary sits at `z = (τ - a)/b` for the
    /// row's `(a, b)`.
    Crossing { tau: f64 },
}

impl PartitionEdge {
    /// The boundary's z location at the row scalars `(a, b)`.
    #[inline]
    pub fn z_at(self, a: f64, b: f64) -> f64 {
        match self {
            Self::Fixed(z) => z,
            Self::Crossing { tau } => (tau - a) / b,
        }
    }
}

#[derive(Clone, Copy, Debug, Eq, PartialEq, Hash)]
struct TailCellMomentCacheKey {
    c0_bits: u64,
    c1_bits: u64,
    endpoint_bits: u64,
    side: i8,
    max_degree: usize,
}

const TAIL_CELL_MOMENT_CACHE_MAX_BYTES: usize = 64 * 1024 * 1024;
const TAIL_CELL_MOMENT_CACHE_MAX_ENTRIES: usize = 262_144;

#[derive(Clone, Copy, Debug, Default, Eq, PartialEq)]
pub struct TailCellMomentCacheStats {
    pub hits: usize,
    pub misses: usize,
    pub entries: usize,
}

impl TailCellMomentCacheStats {
    #[inline]
    pub fn requests(self) -> usize {
        self.hits + self.misses
    }

    #[inline]
    pub fn hit_rate(self) -> f64 {
        let requests = self.requests();
        if requests == 0 {
            0.0
        } else {
            self.hits as f64 / requests as f64
        }
    }
}

/// Affine-tail cell-moment memo.
///
/// Stand-alone instances (`TailCellMomentCache::new()`) are useful when a
/// caller needs deterministic hit/miss bookkeeping that is not polluted by
/// concurrent traffic on the global memo. The production path uses the
/// global instance behind [`evaluate_cell_moments`].
///
/// All methods take `&self`: the LRU is internally synchronized (sharded for
/// the concurrent global memo) and the counters are atomics, so the global
/// instance needs no outer `Mutex`. The previous `OnceLock<Mutex<…>>` wrapper
/// serialized every tail-cell evaluation across all rayon workers of the
/// marginal-slope exact-cache build — the same contention class the sharded
/// per-family cell-moment LRU fix removed.
#[derive(Debug)]
pub struct TailCellMomentCache {
    moments: ByteLruCache<TailCellMomentCacheKey, CellMomentState>,
    in_flight: std::sync::Mutex<
        std::collections::HashMap<
            TailCellMomentCacheKey,
            Arc<std::sync::OnceLock<Result<CellMomentState, String>>>,
        >,
    >,
    hits: std::sync::atomic::AtomicUsize,
    misses: std::sync::atomic::AtomicUsize,
}

impl Default for TailCellMomentCache {
    fn default() -> Self {
        // Tail-cell entries are small (a short moment vector), so sharding
        // the byte/entry budgets is harmless; size the shard count off the
        // worker pool exactly like the per-family cell-moment LRU.
        let shard_count = std::thread::available_parallelism()
            .map(|workers| workers.get().saturating_mul(8))
            .unwrap_or(32)
            .clamp(8, 256);
        Self {
            moments: ByteLruCache::with_max_entries_sharded(
                TAIL_CELL_MOMENT_CACHE_MAX_BYTES,
                TAIL_CELL_MOMENT_CACHE_MAX_ENTRIES,
                shard_count,
            ),
            in_flight: std::sync::Mutex::new(std::collections::HashMap::new()),
            hits: std::sync::atomic::AtomicUsize::new(0),
            misses: std::sync::atomic::AtomicUsize::new(0),
        }
    }
}

impl TailCellMomentCache {
    /// Construct an empty cache. Hits/misses start at zero.
    #[inline]
    pub fn new() -> Self {
        Self::default()
    }

    /// Reset the cache to its empty state. Existing entries are dropped and
    /// the hit/miss counters are zeroed.
    #[inline]
    pub fn clear(&self) {
        self.moments.clear();
        self.in_flight
            .lock()
            .unwrap_or_else(|p| p.into_inner())
            .clear();
        self.hits.store(0, std::sync::atomic::Ordering::Relaxed);
        self.misses.store(0, std::sync::atomic::Ordering::Relaxed);
    }

    /// Snapshot of the cache's current usage stats.
    #[inline]
    pub fn stats(&self) -> TailCellMomentCacheStats {
        TailCellMomentCacheStats {
            hits: self.hits.load(std::sync::atomic::Ordering::Relaxed),
            misses: self.misses.load(std::sync::atomic::Ordering::Relaxed),
            entries: self.moments.len(),
        }
    }

    /// Look up `cell` at `max_degree`, computing and inserting the result on
    /// miss. Cells outside the affine-tail keyset bypass the cache and run
    /// the uncached evaluator directly without touching the counters.
    ///
    /// Stat semantics: every request served from an existing resident entry,
    /// or from a concurrently published entry for the same key, increments
    /// `hits`; a **miss** is counted only for the caller that actually
    /// computes a cold key. The compute happens outside the LRU shard lock,
    /// but an in-flight table coalesces same-key cold races so followers reuse
    /// the leader's published value instead of duplicating work.
    pub fn evaluate(
        &self,
        cell: DenestedCubicCell,
        max_degree: usize,
    ) -> Result<CellMomentState, String> {
        let Some(key) = tail_cell_cache_key(cell, max_degree) else {
            return evaluate_cell_moments_uncached(cell, max_degree);
        };
        if let Some(state) = self.moments.get(&key) {
            self.hits.fetch_add(1, std::sync::atomic::Ordering::Relaxed);
            return Ok(state);
        }

        let (slot, leader) = {
            let mut in_flight = self.in_flight.lock().unwrap_or_else(|p| p.into_inner());
            if let Some(slot) = in_flight.get(&key) {
                (Arc::clone(slot), false)
            } else {
                let slot = Arc::new(std::sync::OnceLock::new());
                in_flight.insert(key, Arc::clone(&slot));
                (slot, true)
            }
        };

        if !leader {
            let state = slot.wait().clone()?;
            self.hits.fetch_add(1, std::sync::atomic::Ordering::Relaxed);
            return Ok(state);
        }

        let state = evaluate_cell_moments_uncached(cell, max_degree);
        if let Ok(state) = &state {
            self.moments.insert(key, state.clone());
            self.hits.fetch_add(1, std::sync::atomic::Ordering::Relaxed);
        }
        self.misses
            .fetch_add(1, std::sync::atomic::Ordering::Relaxed);
        if let Err(existing_state) = slot.set(state.clone()) {
            std::mem::drop(existing_state);
        }
        self.in_flight
            .lock()
            .unwrap_or_else(|p| p.into_inner())
            .remove(&key);
        state
    }
}

static TAIL_CELL_MOMENT_CACHE: std::sync::OnceLock<TailCellMomentCache> =
    std::sync::OnceLock::new();
static TAIL_CELL_MOMENT_CACHE_ENABLED: std::sync::atomic::AtomicBool =
    std::sync::atomic::AtomicBool::new(true);

fn tail_cell_moment_cache() -> &'static TailCellMomentCache {
    TAIL_CELL_MOMENT_CACHE.get_or_init(TailCellMomentCache::default)
}

#[inline]
fn tail_cell_cache_key(
    cell: DenestedCubicCell,
    max_degree: usize,
) -> Option<TailCellMomentCacheKey> {
    if cell.c2.abs() > NORMALIZED_CELL_BRANCH_TOL || cell.c3.abs() > NORMALIZED_CELL_BRANCH_TOL {
        return None;
    }
    match (!cell.left.is_finite(), !cell.right.is_finite()) {
        (true, false) if cell.right.is_finite() => Some(TailCellMomentCacheKey {
            c0_bits: cell.c0.to_bits(),
            c1_bits: cell.c1.to_bits(),
            endpoint_bits: cell.right.to_bits(),
            side: -1,
            max_degree,
        }),
        (false, true) if cell.left.is_finite() => Some(TailCellMomentCacheKey {
            c0_bits: cell.c0.to_bits(),
            c1_bits: cell.c1.to_bits(),
            endpoint_bits: cell.left.to_bits(),
            side: 1,
            max_degree,
        }),
        _ => None,
    }
}

pub fn set_tail_cell_moment_cache_enabled(enabled: bool) {
    TAIL_CELL_MOMENT_CACHE_ENABLED.store(enabled, std::sync::atomic::Ordering::Relaxed);
}

pub fn reset_tail_cell_moment_cache() {
    tail_cell_moment_cache().clear();
}

pub fn tail_cell_moment_cache_stats() -> TailCellMomentCacheStats {
    tail_cell_moment_cache().stats()
}

#[derive(Clone, Copy, Debug, Eq)]
pub struct CellFingerprint {
    c0: u64,
    c1: u64,
    c2: u64,
    c3: u64,
    left: u64,
    right: u64,
}

impl CellFingerprint {
    #[inline]
    pub fn new(cell: DenestedCubicCell) -> Self {
        Self {
            c0: cell.c0.to_bits(),
            c1: cell.c1.to_bits(),
            c2: cell.c2.to_bits(),
            c3: cell.c3.to_bits(),
            left: cell.left.to_bits(),
            right: cell.right.to_bits(),
        }
    }
}

impl PartialEq for CellFingerprint {
    #[inline]
    fn eq(&self, other: &Self) -> bool {
        self.c0 == other.c0
            && self.c1 == other.c1
            && self.c2 == other.c2
            && self.c3 == other.c3
            && self.left == other.left
            && self.right == other.right
    }
}

impl Hash for CellFingerprint {
    #[inline]
    fn hash<H: Hasher>(&self, state: &mut H) {
        self.c0.hash(state);
        self.c1.hash(state);
        self.c2.hash(state);
        self.c3.hash(state);
        self.left.hash(state);
        self.right.hash(state);
    }
}

#[derive(Clone, Debug, Default, PartialEq)]
pub struct CachedCellMoments {
    /// Regular (value) cell moments, populated by
    /// `evaluate_cell_moments_cached`. None when only derivative moments
    /// have been cached for this cell. Wrapped in `Arc` so `ByteLruCache`
    /// returns lookups through cheap refcount bumps instead of deep-cloning
    /// the inline `SmallVec<[f64; 10]>` (which spills on every degree-`>= 10`
    /// request) on every hot-path LRU hit.
    state: Option<Arc<CellMomentState>>,
    /// Derivative moments, populated by
    /// `evaluate_cell_derivative_moments_cached`. None when only value
    /// moments have been cached for this cell. Both variants share the
    /// same `CellFingerprint` key so derivative-only callers do not evict
    /// pre-cached value entries and vice versa. Same `Arc` wrapping rationale
    /// as `state` above.
    derivative_state: Option<Arc<CellDerivativeMomentState>>,
}

impl CachedCellMoments {
    #[inline]
    pub fn new(state: Arc<CellMomentState>) -> Self {
        Self {
            state: Some(state),
            derivative_state: None,
        }
    }

    #[inline]
    pub fn new_derivative(state: Arc<CellDerivativeMomentState>) -> Self {
        Self {
            state: None,
            derivative_state: Some(state),
        }
    }

    #[inline]
    pub fn state_for_degree(&self, max_degree: usize) -> Option<CellMomentState> {
        let state = self.state.as_ref()?;
        if state.moments.len().saturating_sub(1) < max_degree {
            return None;
        }
        // Cached `Arc<CellMomentState>` is shared across LRU hits, so we
        // cannot reuse the inner vector in place. Clone the underlying state
        // and (rarely) truncate down to the requested degree to honour the
        // public moment-length contract.
        let mut state = (**state).clone();
        state.moments.truncate(max_degree + 1);
        Some(state)
    }

    #[inline]
    pub fn derivative_state_for_degree(
        &self,
        max_degree: usize,
    ) -> Option<CellDerivativeMomentState> {
        let state = self.derivative_state.as_ref()?;
        if state.moments.len().saturating_sub(1) < max_degree {
            return None;
        }
        // See `state_for_degree`: shared `Arc` forces an inner clone here.
        let mut state = (**state).clone();
        state.moments.truncate(max_degree + 1);
        Some(state)
    }

    #[inline]
    pub fn with_value(mut self, state: Arc<CellMomentState>) -> Self {
        self.state = Some(state);
        self
    }

    #[inline]
    pub fn with_derivative(mut self, state: Arc<CellDerivativeMomentState>) -> Self {
        self.derivative_state = Some(state);
        self
    }
}

impl ResidentBytes for CachedCellMoments {
    fn resident_bytes(&self) -> usize {
        let value_bytes = self
            .state
            .as_ref()
            .map_or(0, |state| state.resident_bytes());
        let derivative_bytes = self
            .derivative_state
            .as_ref()
            .map_or(0, |state| state.resident_bytes());
        std::mem::size_of::<Self>()
            .saturating_add(value_bytes)
            .saturating_add(derivative_bytes)
    }
}

#[derive(Debug, Default)]
pub struct CellMomentCacheStats {
    hits: AtomicU64,
    misses: AtomicU64,
}

impl CellMomentCacheStats {
    #[inline]
    pub fn snapshot(&self) -> (u64, u64) {
        (
            self.hits.load(Ordering::Relaxed),
            self.misses.load(Ordering::Relaxed),
        )
    }

    #[inline]
    pub fn hit_rate_delta(&self, before: (u64, u64)) -> (u64, u64, f64) {
        let (hits, misses) = self.snapshot();
        let dh = hits.saturating_sub(before.0);
        let dm = misses.saturating_sub(before.1);
        let total = dh + dm;
        let rate = if total == 0 {
            0.0
        } else {
            dh as f64 / total as f64
        };
        (dh, dm, rate)
    }
}

pub type CellMomentLruCache = ByteLruCache<CellFingerprint, CachedCellMoments>;

pub const CELL_MOMENT_INLINE_CAPACITY: usize = 10;

pub type CellMomentVec = SmallVec<[f64; CELL_MOMENT_INLINE_CAPACITY]>;

#[derive(Clone, Debug, PartialEq)]
pub struct CellMomentState {
    pub branch: ExactCellBranch,
    pub value: f64,
    pub moments: CellMomentVec,
}

impl ResidentBytes for CellMomentState {
    fn resident_bytes(&self) -> usize {
        let spilled_bytes = if self.moments.spilled() {
            self.moments
                .capacity()
                .saturating_mul(std::mem::size_of::<f64>())
        } else {
            0
        };
        std::mem::size_of::<Self>().saturating_add(spilled_bytes)
    }
}

#[derive(Clone, Debug, PartialEq)]
pub struct CellDerivativeMomentState {
    pub branch: ExactCellBranch,
    pub moments: CellMomentVec,
}

impl ResidentBytes for CellDerivativeMomentState {
    fn resident_bytes(&self) -> usize {
        let spilled_bytes = if self.moments.spilled() {
            self.moments
                .capacity()
                .saturating_mul(std::mem::size_of::<f64>())
        } else {
            0
        };
        std::mem::size_of::<Self>().saturating_add(spilled_bytes)
    }
}

#[derive(Clone, Copy, Debug, PartialEq)]
pub struct CellMomentStateRef<'a> {
    pub branch: ExactCellBranch,
    pub value: f64,
    pub moments: &'a [f64],
}

#[derive(Clone, Debug)]
pub struct CellMomentScratch {
    moments: Vec<f64>,
}

impl Default for CellMomentScratch {
    fn default() -> Self {
        // Pre-size to the codebase's max moment degree so steady-state
        // `prepare_moments` calls never reallocate. Calls with `len`
        // exceeding this still reserve lazily.
        Self {
            moments: Vec::with_capacity(MAX_AFFINE_ANCHOR_DEGREE + 1),
        }
    }
}

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

    pub fn with_capacity(max_degree: usize) -> Self {
        Self {
            moments: Vec::with_capacity(max_degree + 1),
        }
    }

    #[inline]
    fn prepare_moments(&mut self, len: usize) -> &mut [f64] {
        if self.moments.capacity() < len {
            CELL_MOMENT_REALLOCS.fetch_add(1, std::sync::atomic::Ordering::Relaxed);
            self.moments.reserve(len - self.moments.capacity());
        }
        // Grow monotonically: shorter requests should not truncate the backing
        // storage and then zero the old tail when a later request grows again.
        // Only the active prefix is scratch for this evaluation.
        if self.moments.len() < len {
            self.moments.resize(len, 0.0);
        }
        let out = &mut self.moments[..len];
        out.fill(0.0);
        out
    }
}

/// Counter for moment-buffer reallocations in `prepare_moments`. Production
/// code increments this on every buffer growth; the test mod inspects it to
/// assert the steady-state hot loop allocates exactly once per row buffer.
pub(crate) static CELL_MOMENT_REALLOCS: std::sync::atomic::AtomicUsize =
    std::sync::atomic::AtomicUsize::new(0);

/// Canonical 20-point Gauss–Legendre nodes on [-1, 1] (Abramowitz & Stegun
/// 25.4), tabulated to f64 precision. Used here for the Drezner–Wesolowsky
/// bivariate normal CDF representation — 20 points give >30-digit accuracy for
/// the smooth arcsin-transformed integrand, ensuring the BVN value is exact to
/// f64 precision for all (h, k, ρ) — and shared with the cubic-cell B-spline
/// moment parity gate in [`crate::gpu_kernels::cubic_bspline_moments`].
pub const GL20_NODES: [f64; 20] = [
    -0.993_128_599_185_094_9,
    -0.963_971_927_277_913_8,
    -0.912_234_428_251_326,
    -0.839_116_971_822_218_8,
    -0.746_331_906_460_150_8,
    -0.636_053_680_726_515,
    -0.510_867_001_950_827_1,
    -0.373_706_088_715_419_6,
    -0.227_785_851_141_645_1,
    -0.076_526_521_133_497_33,
    0.076_526_521_133_497_33,
    0.227_785_851_141_645_1,
    0.373_706_088_715_419_6,
    0.510_867_001_950_827_1,
    0.636_053_680_726_515,
    0.746_331_906_460_150_8,
    0.839_116_971_822_218_8,
    0.912_234_428_251_326,
    0.963_971_927_277_913_8,
    0.993_128_599_185_094_9,
];

/// Companion weights to [`GL20_NODES`]. Symmetric, summing to 2.
pub const GL20_WEIGHTS: [f64; 20] = [
    0.017_614_007_139_152_12,
    0.040_601_429_800_386_94,
    0.062_672_048_334_109_06,
    0.083_276_741_576_704_75,
    0.101_930_119_817_240_4,
    0.118_194_531_961_518_4,
    0.131_688_638_449_176_6,
    0.142_096_109_318_382_1,
    0.149_172_986_472_603_7,
    0.152_753_387_130_725_9,
    0.152_753_387_130_725_9,
    0.149_172_986_472_603_7,
    0.142_096_109_318_382_1,
    0.131_688_638_449_176_6,
    0.118_194_531_961_518_4,
    0.101_930_119_817_240_4,
    0.083_276_741_576_704_75,
    0.062_672_048_334_109_06,
    0.040_601_429_800_386_94,
    0.017_614_007_139_152_12,
];

/// Provenance-tagged breakpoint dedup: sorts ascending and merges entries
/// coinciding within 1e-12, but when a fixed score break and a link-knot
/// crossing coincide (the kink configuration), the surviving entry keeps
/// the `Fixed` tag — a deterministic choice; the z location is identical
/// either way.
fn dedup_sorted_tagged_breakpoints(points: &mut Vec<(f64, PartitionEdge)>) {
    points.sort_by(|lhs, rhs| {
        lhs.0
            .partial_cmp(&rhs.0)
            .unwrap_or(std::cmp::Ordering::Equal)
    });
    points.dedup_by(|lhs, rhs| {
        let coincide = if lhs.0 == rhs.0 {
            true
        } else if lhs.0.is_finite() && rhs.0.is_finite() {
            (lhs.0 - rhs.0).abs() <= 1e-12
        } else {
            false
        };
        if coincide && matches!(lhs.1, PartitionEdge::Fixed(_)) {
            // `dedup_by` keeps `rhs` (the earlier element) — propagate the
            // Fixed tag onto the survivor.
            rhs.1 = lhs.1;
        }
        coincide
    });
}

#[inline]
pub fn interval_probe_point(left: f64, right: f64) -> Result<f64, String> {
    if !(left < right) {
        return Err(CubicCellKernelError::invalid_interval(format!(
            "interval probe requires ordered bounds, got [{left}, {right}]"
        ))
        .into());
    }
    if left.is_finite() && right.is_finite() {
        Ok(0.5 * (left + right))
    } else if left == f64::NEG_INFINITY && right == f64::INFINITY {
        Ok(0.0)
    } else if left == f64::NEG_INFINITY && right.is_finite() {
        Ok(right - 1.0)
    } else if left.is_finite() && right == f64::INFINITY {
        Ok(left + 1.0)
    } else {
        Err(CubicCellKernelError::invalid_interval(format!(
            "interval probe requires finite bounds or full infinities, got [{left}, {right}]"
        ))
        .into())
    }
}

#[inline]
pub fn quartic_qprime_coefficients(c0: f64, c1: f64, c2: f64) -> [f64; 4] {
    [
        c0 * c1,
        1.0 + c1 * c1 + 2.0 * c0 * c2,
        3.0 * c1 * c2,
        2.0 * c2 * c2,
    ]
}

#[inline]
pub fn sextic_qprime_coefficients(c0: f64, c1: f64, c2: f64, c3: f64) -> [f64; 6] {
    [
        c0 * c1,
        1.0 + c1 * c1 + 2.0 * c0 * c2,
        3.0 * c0 * c3 + 3.0 * c1 * c2,
        4.0 * c1 * c3 + 2.0 * c2 * c2,
        5.0 * c2 * c3,
        3.0 * c3 * c3,
    ]
}

/// Boundary term `right^n · exp(−q(right)) − left^n · exp(−q(left))` used by
/// the moment recurrences. Takes precomputed `left^n` and `right^n` so callers
/// can roll the powers across a recurrence — each iteration becomes one
/// multiply instead of a fresh `powi(n)`.
#[inline]
fn moment_boundary_term_with_powers(
    cell: DenestedCubicCell,
    left_pow_n: f64,
    right_pow_n: f64,
) -> f64 {
    let left_term = if cell.left.is_infinite() {
        0.0
    } else {
        left_pow_n * (-cell.q(cell.left)).exp()
    };
    let right_term = if cell.right.is_infinite() {
        0.0
    } else {
        right_pow_n * (-cell.q(cell.right)).exp()
    };
    right_term - left_term
}

#[inline]
fn base_moments_match_direct(base: &[f64], direct: &[f64]) -> bool {
    base.iter()
        .zip(direct.iter())
        .all(|(&lhs, &rhs)| (lhs - rhs).abs() <= 1e-10 * (1.0 + lhs.abs().max(rhs.abs())))
}

#[inline]
fn direct_non_affine_moments_if_base_matches(
    cell: DenestedCubicCell,
    base: &[f64],
    max_degree: usize,
) -> Option<Vec<f64>> {
    if !cell.left.is_finite() || !cell.right.is_finite() {
        return None;
    }
    // When the supplied base moments are the actual moments of this fixed
    // finite cell, prefer the same quadrature-backed evaluator used by the
    // public non-affine moment path.  The algebraic raising recurrence is kept
    // below for callers that intentionally pass symbolic or otherwise
    // non-cell-consistent bases, but repeatedly dividing by the quartic/sextic
    // leading coefficient can amplify harmless base-roundoff into high-order
    // moment error.
    let (moments, _) = evaluate_non_affine_cell_simd::<false>(cell, max_degree);
    if base_moments_match_direct(base, &moments) {
        Some(moments.into_vec())
    } else {
        None
    }
}

pub fn reduce_quartic_moments(
    cell: DenestedCubicCell,
    base_m0_m2: [f64; 3],
    max_degree: usize,
) -> Result<Vec<f64>, String> {
    if max_degree <= 2 {
        return Ok(base_m0_m2[..=max_degree].to_vec());
    }
    if let Some(moments) = direct_non_affine_moments_if_base_matches(cell, &base_m0_m2, max_degree)
    {
        return Ok(moments);
    }
    let d = quartic_qprime_coefficients(cell.c0, cell.c1, cell.c2);
    let lead = d[3];
    if !lead.is_finite() || lead.abs() <= 1e-18 {
        return Err(CubicCellKernelError::invalid_cell_shape(format!(
            "quartic moment reduction requires nonzero leading coefficient, got {lead:.3e}"
        ))
        .into());
    }
    let mut moments = vec![0.0; max_degree + 1];
    moments[0] = base_m0_m2[0];
    moments[1] = base_m0_m2[1];
    moments[2] = base_m0_m2[2];
    // Roll left^n / right^n across the recurrence rather than calling
    // `powi(n)` each iteration. Skip the multiply when an endpoint is
    // infinite — the boundary helper ignores the power in that case, and
    // ∞·0 would produce a NaN we'd then have to mask off anyway.
    let left_finite = cell.left.is_finite();
    let right_finite = cell.right.is_finite();
    let mut left_pow_n = if left_finite { 1.0 } else { 0.0 };
    let mut right_pow_n = if right_finite { 1.0 } else { 0.0 };
    for n in 0..=(max_degree - 3) {
        let b_n = moment_boundary_term_with_powers(cell, left_pow_n, right_pow_n);
        let mut numer = if n == 0 {
            0.0
        } else {
            (n as f64) * moments[n - 1]
        };
        for j in 0..=2 {
            numer -= d[j] * moments[n + j];
        }
        numer -= b_n;
        moments[n + 3] = numer / lead;
        if left_finite {
            left_pow_n *= cell.left;
        }
        if right_finite {
            right_pow_n *= cell.right;
        }
    }
    Ok(moments)
}

pub fn reduce_sextic_moments(
    cell: DenestedCubicCell,
    base_m0_m4: [f64; 5],
    max_degree: usize,
) -> Result<Vec<f64>, String> {
    if max_degree <= 4 {
        return Ok(base_m0_m4[..=max_degree].to_vec());
    }
    if let Some(moments) = direct_non_affine_moments_if_base_matches(cell, &base_m0_m4, max_degree)
    {
        return Ok(moments);
    }
    let d = sextic_qprime_coefficients(cell.c0, cell.c1, cell.c2, cell.c3);
    let lead = d[5];
    if !lead.is_finite() {
        return Err(CubicCellKernelError::invalid_cell_shape(format!(
            "sextic moment reduction encountered non-finite leading coefficient: {lead:.3e}"
        ))
        .into());
    }
    if let Some(lower_branch) = degenerate_sextic_branch(cell, lead)? {
        if lower_branch == ExactCellBranch::Quartic {
            return evaluate_non_affine_cell_state(
                DenestedCubicCell { c3: 0.0, ..cell },
                ExactCellBranch::Quartic,
                max_degree,
            )
            .map(|state| state.moments.into_vec());
        }
        return evaluate_affine_cell_state(
            DenestedCubicCell {
                left: cell.left,
                right: cell.right,
                c0: cell.c0,
                c1: cell.c1,
                c2: 0.0,
                c3: 0.0,
            },
            max_degree,
        )
        .map(|state| state.moments.into_vec());
    }
    let mut moments = vec![0.0; max_degree + 1];
    for (idx, value) in base_m0_m4.into_iter().enumerate() {
        moments[idx] = value;
    }
    let left_finite = cell.left.is_finite();
    let right_finite = cell.right.is_finite();
    let mut left_pow_n = if left_finite { 1.0 } else { 0.0 };
    let mut right_pow_n = if right_finite { 1.0 } else { 0.0 };
    for n in 0..=(max_degree - 5) {
        let b_n = moment_boundary_term_with_powers(cell, left_pow_n, right_pow_n);
        let mut numer = if n == 0 {
            0.0
        } else {
            (n as f64) * moments[n - 1]
        };
        for j in 0..=4 {
            numer -= d[j] * moments[n + j];
        }
        numer -= b_n;
        moments[n + 5] = numer / lead;
        if left_finite {
            left_pow_n *= cell.left;
        }
        if right_finite {
            right_pow_n *= cell.right;
        }
    }
    Ok(moments)
}

#[inline]
pub fn cell_first_derivative_from_moments(
    derivative_coefficients: &[f64],
    moments: &[f64],
) -> Result<f64, String> {
    let value = moment_dot_with_coefficients(derivative_coefficients, moments, "first derivative")?;
    Ok(value * INV_TWO_PI)
}

/// Maximum moment index (i.e. `max_degree` passed to
/// `evaluate_cell_moments`) required to evaluate
/// `cell_first_derivative_from_moments(derivative_coefficients, moments)`.
///
/// Callers must request at least `cell_first_derivative_required_max_degree(
/// derivative_coefficients)` so the moment dot is well-defined; #321 was
/// caused by hardcoding a smaller value at one call site.
#[inline]
pub fn cell_first_derivative_required_max_degree(derivative_coefficients: &[f64]) -> usize {
    derivative_coefficients.len().saturating_sub(1)
}

/// Maximum moment index required by `cell_second_derivative_from_moments`.
///
/// Mirrors the kernel's internal `needed = max(second_deg, product_deg) + 1`
/// computation, but returned as `max_degree` (i.e. `needed - 1`) so it lines
/// up with the `evaluate_cell_moments(cell, max_degree)` argument convention.
/// The contraction folds an inner cubic `eta` (always degree 3) with the two
/// first-coefficient slices and the second-coefficient slice; the +3 below is
/// the cubic-cell eta polynomial.
#[inline]
pub fn cell_second_derivative_required_max_degree(
    first_coefficients_r: &[f64],
    first_coefficients_s: &[f64],
    second_coefficients_rs: &[f64],
) -> usize {
    let second_degree = second_coefficients_rs.len().saturating_sub(1);
    let product_degree = first_coefficients_r.len().saturating_sub(1)
        + first_coefficients_s.len().saturating_sub(1)
        + 3;
    second_degree.max(product_degree)
}

#[inline]
pub fn cell_polynomial_integral_from_moments(
    polynomial_coefficients: &[f64],
    moments: &[f64],
    label: &str,
) -> Result<f64, String> {
    let value = moment_dot_with_coefficients(polynomial_coefficients, moments, label)?;
    Ok(value * INV_TWO_PI)
}

#[inline]
pub fn cell_second_derivative_from_moments(
    cell: DenestedCubicCell,
    first_coefficients_r: &[f64],
    first_coefficients_s: &[f64],
    second_coefficients_rs: &[f64],
    moments: &[f64],
) -> Result<f64, String> {
    let second_degree = second_coefficients_rs.len().saturating_sub(1);
    let product_degree = first_coefficients_r.len().saturating_sub(1)
        + first_coefficients_s.len().saturating_sub(1)
        + 3;
    let needed = second_degree.max(product_degree) + 1;
    if needed > moments.len() {
        return Err(CubicCellKernelError::insufficient_moments(format!(
            "insufficient reduced moments for second derivative: need {}, have {}",
            needed,
            moments.len()
        ))
        .into());
    }
    let second_term = moment_dot_with_coefficients_unchecked(second_coefficients_rs, moments);
    // Fold `Σ_{e,i,j} eta[e]·r[i]·s[j]·moments[e+i+j]` into a single dot
    // against `moments`. Convolving `eta ⊗ r ⊗ s` first turns the original
    // `len(eta)·len(r)·len(s)` triple loop (typically 4·4·4 = 64 mul-adds
    // per call) into `len(eta)·len(r) + (len(eta)+len(r)-1)·len(s) +
    // len(out)` ≈ 16 + 28 + 10 = 54 mul-adds, with the inner loops now in
    // straight-line FMA-friendly form.
    let cubic = [cell.c0, cell.c1, cell.c2, cell.c3];
    // Capacity bound: cubic (4) + first_r (≤MAX) + first_s (≤MAX) - 2.
    // First-coefficient slices are passed in as `[f64; 4]` from every
    // production caller; sizing to 32 covers any realistic test input.
    const SCRATCH: usize = 32;
    let mut eta_r = [0.0_f64; SCRATCH];
    let mut eta_rs = [0.0_f64; SCRATCH];
    let er_len = poly_conv_into(&cubic, first_coefficients_r, &mut eta_r);
    let ers_len = poly_conv_into(&eta_r[..er_len], first_coefficients_s, &mut eta_rs);
    let mut eta_term = 0.0;
    for k in 0..ers_len {
        eta_term = eta_rs[k].mul_add(moments[k], eta_term);
    }
    Ok((second_term - eta_term) * INV_TWO_PI)
}

/// Pointwise value of the cell second-derivative integrand
/// `(∂²/∂r∂s) exp(-q(z))/2π` at a single `z`, evaluated from the SAME
/// `(r, s, rs)` coefficient polynomials the moment reduction
/// [`cell_second_derivative_from_moments`] integrates:
///
/// ```text
///   F_rs(z) = ( c_rs(z) - η(z)·c_r(z)·c_s(z) ) · exp(-q(z)) · 1/2π ,
/// ```
///
/// with `c_•(z) = Σ_k coeff_•[k]·zᵏ`, `η(z)` the cell cubic, and
/// `q(z) = ½(z² + η(z)²)`. This is the integrand whose `[cell.left,
/// cell.right]` integral the from-moments form returns — needed for the
/// Leibniz boundary term when a cell edge (a link-knot crossing
/// `z=(τ-a)/b`) moves with a parameter (the slope `b`): the directional
/// derivative of `∫_{z_L}^{z_R} F_rs dz` picks up
/// `F_rs(z_R)·z_R'(dir) - F_rs(z_L)·z_L'(dir)` on top of the fixed-domain
/// part. Coefficient sign convention matches the simpson reference
/// (`numeric_ab`): pass the ACTUAL derivative-coefficient polynomials
/// `∂c/∂r` etc. (not the negated `neg_dc_d•` the moment path consumes).
#[inline]
pub fn cell_second_derivative_boundary_integrand(
    cell: DenestedCubicCell,
    first_coefficients_r: &[f64],
    first_coefficients_s: &[f64],
    second_coefficients_rs: &[f64],
    z: f64,
) -> f64 {
    let eta = cell.eta(z);
    let c_r = poly_eval_at(first_coefficients_r, z);
    let c_s = poly_eval_at(first_coefficients_s, z);
    let c_rs = poly_eval_at(second_coefficients_rs, z);
    (c_rs - eta * c_r * c_s) * (-cell.q(z)).exp() * INV_TWO_PI
}

/// Pointwise value of the cell third-derivative integrand
/// `(∂³/∂r∂s∂t) exp(-q(z))/2π` at a single `z`, evaluated from the same
/// `(r, s, t, rs, rt, st, rst)` coefficient polynomials that
/// [`cell_third_derivative_from_moments`] integrates:
///
/// ```text
/// F_rst(z) = (
///     c_rst(z)
///   - η(z)·(c_rs(z)c_t(z) + c_rt(z)c_s(z) + c_st(z)c_r(z))
///   + (η(z)² - 1)·c_r(z)c_s(z)c_t(z)
/// ) · exp(-q(z)) · 1/2π .
/// ```
///
/// This is the boundary value for differentiating an already-third-order
/// fixed-domain integral with respect to a moving edge. The sign convention is
/// intentionally identical to [`cell_third_derivative_from_moments`]: callers
/// must pass the coefficient slices in the convention of the integral they are
/// differentiating. In particular, survival/probit paths that integrate the
/// jointly negated cell and coefficient slices must evaluate this boundary
/// integrand with the same joint negation; evaluating an un-negated boundary for
/// a negated fixed-domain integral flips the sign of this odd-order integrand.
#[inline]
pub fn cell_third_derivative_boundary_integrand(
    cell: DenestedCubicCell,
    first_coefficients_r: &[f64],
    first_coefficients_s: &[f64],
    first_coefficients_t: &[f64],
    second_coefficients_rs: &[f64],
    second_coefficients_rt: &[f64],
    second_coefficients_st: &[f64],
    third_coefficients_rst: &[f64],
    z: f64,
) -> f64 {
    let eta = cell.eta(z);
    let c_r = poly_eval_at(first_coefficients_r, z);
    let c_s = poly_eval_at(first_coefficients_s, z);
    let c_t = poly_eval_at(first_coefficients_t, z);
    let c_rs = poly_eval_at(second_coefficients_rs, z);
    let c_rt = poly_eval_at(second_coefficients_rt, z);
    let c_st = poly_eval_at(second_coefficients_st, z);
    let c_rst = poly_eval_at(third_coefficients_rst, z);
    let amplitude =
        c_rst - eta * (c_rs * c_t + c_rt * c_s + c_st * c_r) + (eta * eta - 1.0) * c_r * c_s * c_t;
    amplitude * (-cell.q(z)).exp() * INV_TWO_PI
}

/// Pointwise value of the density-weighted integrand `g(z)·exp(-q(z))/2π` at a
/// single `z`, for an arbitrary integrand polynomial `g`.
///
/// This is the boundary value needed for the moving-domain (Leibniz) term of a
/// density-normalization integral `∫ g(z)·exp(-q(z))/2π dz` whose cell edge is a
/// link-knot crossing `z=(τ-a)/b` that moves with a parameter direction: the
/// directional derivative of the integral picks up
/// `g(z_R)·w(z_R)·z_R'(dir) - g(z_L)·w(z_L)·z_L'(dir)` on top of the
/// fixed-domain part, with `w(z)=exp(-q(z))/2π` the same weight the moment
/// reductions integrate. Unlike the Hessian-integral boundary term (which is
/// shared by adjacent cells and cancels across each interior knot), the
/// ln-density integrand `D_t`/`D_t,uv` carries a non-shared `g`, so this
/// Leibniz term does NOT cancel and must be added (gam#932/#979).
pub fn cell_density_boundary_integrand(cell: DenestedCubicCell, g: &[f64], z: f64) -> f64 {
    poly_eval_at(g, z) * (-cell.q(z)).exp() * INV_TWO_PI
}

/// Horner evaluation of `Σ_k coefficients[k]·zᵏ`.
#[inline]
fn poly_eval_at(coefficients: &[f64], z: f64) -> f64 {
    let mut acc = 0.0_f64;
    for &c in coefficients.iter().rev() {
        acc = acc.mul_add(z, c);
    }
    acc
}

#[inline]
fn moment_dot_with_coefficients(
    coefficients: &[f64],
    moments: &[f64],
    label: &str,
) -> Result<f64, String> {
    if coefficients.len() > moments.len() {
        return Err(CubicCellKernelError::insufficient_moments(format!(
            "insufficient reduced moments for {label}: need {}, have {}",
            coefficients.len(),
            moments.len()
        ))
        .into());
    }
    Ok(moment_dot_with_coefficients_unchecked(
        coefficients,
        moments,
    ))
}

#[inline]
fn moment_dot_with_coefficients_unchecked(coefficients: &[f64], moments: &[f64]) -> f64 {
    let mut acc = 0.0;
    for (idx, &coeff) in coefficients.iter().enumerate() {
        acc = coeff.mul_add(moments[idx], acc);
    }
    acc
}

/// Convolve two polynomial coefficient slices into a fixed-capacity output
/// buffer. Returns the populated length (`lhs.len() + rhs.len() - 1` when
/// both are non-empty). The buffer's tail (beyond the returned length) is
/// not zeroed; callers must use only the returned prefix.
///
/// Used by the multi-derivative reductions to fold `eta · r · s · …` triple
/// and quadruple sums into a single moment dot, eliminating the
/// `O(deg^3)`/`O(deg^4)` inner-loop work that dominated the
/// `cell_*_derivative_from_moments` hot leaves on large-scale fits.
#[inline]
fn poly_conv_into(lhs: &[f64], rhs: &[f64], out: &mut [f64]) -> usize {
    if lhs.is_empty() || rhs.is_empty() {
        return 0;
    }
    let len = lhs.len() + rhs.len() - 1;
    assert!(out.len() >= len);
    for slot in out[..len].iter_mut() {
        *slot = 0.0;
    }
    for (i, &lv) in lhs.iter().enumerate() {
        for (j, &rv) in rhs.iter().enumerate() {
            out[i + j] = lv.mul_add(rv, out[i + j]);
        }
    }
    len
}

#[inline]
fn require_moments_degree(
    required_degree: usize,
    moments: &[f64],
    label: &str,
) -> Result<(), String> {
    if required_degree >= moments.len() {
        return Err(CubicCellKernelError::insufficient_moments(format!(
            "insufficient reduced moments for {label}: need {}, have {}",
            required_degree + 1,
            moments.len()
        ))
        .into());
    }
    Ok::<(), _>(())
}

#[inline]
fn require_scratch_capacity(
    required_len: usize,
    capacity: usize,
    label: &str,
) -> Result<(), String> {
    if required_len > capacity {
        return Err(CubicCellKernelError::insufficient_moments(format!(
            "{label} polynomial convolution scratch too small: need {required_len}, have {capacity}"
        ))
        .into());
    }
    Ok::<(), _>(())
}

#[inline]
fn convolution_chain_len(lengths: &[usize]) -> usize {
    if lengths.is_empty() || lengths.contains(&0) {
        0
    } else {
        lengths.iter().sum::<usize>() - (lengths.len() - 1)
    }
}

#[inline]
fn first_coefficients_degree(label: &str, coefficients: &[f64]) -> Result<usize, String> {
    coefficients
        .len()
        .checked_sub(1)
        .ok_or_else(|| format!("{label} first-derivative coefficients must be non-empty"))
}

#[inline]
pub fn cell_third_derivative_from_moments(
    cell: DenestedCubicCell,
    first_coefficients_r: &[f64],
    first_coefficients_s: &[f64],
    first_coefficients_t: &[f64],
    second_coefficients_rs: &[f64],
    second_coefficients_rt: &[f64],
    second_coefficients_st: &[f64],
    third_coefficients_rst: &[f64],
    moments: &[f64],
) -> Result<f64, String> {
    let eta = [cell.c0, cell.c1, cell.c2, cell.c3];
    let r_degree = first_coefficients_degree("r", first_coefficients_r)?;
    let s_degree = first_coefficients_degree("s", first_coefficients_s)?;
    let t_degree = first_coefficients_degree("t", first_coefficients_t)?;
    let second_sum_degree = [
        second_coefficients_rs.len() + first_coefficients_t.len(),
        second_coefficients_rt.len() + first_coefficients_s.len(),
        second_coefficients_st.len() + first_coefficients_r.len(),
    ]
    .into_iter()
    .max()
    .unwrap_or(0)
    .saturating_sub(1);
    let triple_product_degree = r_degree + s_degree + t_degree;
    let needed = (third_coefficients_rst.len().saturating_sub(1))
        .max(3 + second_sum_degree)
        .max(6 + triple_product_degree);
    require_moments_degree(needed, moments, "third derivative")?;

    let third_term = moment_dot_with_coefficients_unchecked(third_coefficients_rst, moments);

    // This is a deliberately serial leaf kernel: each call performs only a
    // handful of fixed-size polynomial convolutions, so Rayon fan-out belongs
    // at the surrounding row/cell batch level rather than inside this hot path.
    const SCRATCH: usize = 32;
    let max_linear_conv_len = [
        convolution_chain_len(&[
            eta.len(),
            second_coefficients_rs.len(),
            first_coefficients_t.len(),
        ]),
        convolution_chain_len(&[
            eta.len(),
            second_coefficients_rt.len(),
            first_coefficients_s.len(),
        ]),
        convolution_chain_len(&[
            eta.len(),
            second_coefficients_st.len(),
            first_coefficients_r.len(),
        ]),
    ]
    .into_iter()
    .max()
    .unwrap_or(0);
    let max_cubic_conv_len = convolution_chain_len(&[
        7,
        first_coefficients_r.len(),
        first_coefficients_s.len(),
        first_coefficients_t.len(),
    ]);
    require_scratch_capacity(
        max_linear_conv_len.max(max_cubic_conv_len),
        SCRATCH,
        "third derivative",
    )?;
    let mut buf_a = [0.0_f64; SCRATCH];
    let mut buf_b = [0.0_f64; SCRATCH];

    // eta_second_term = Σ over (rs⊗t, rt⊗s, st⊗r) of eta⊗product · moments.
    // Fold each of the three triple sums into a single moment dot.
    let mut eta_second_term = 0.0;
    let conv_dot = |first: &[f64],
                    second: &[f64],
                    buf_a: &mut [f64; SCRATCH],
                    buf_b: &mut [f64; SCRATCH]|
     -> f64 {
        let m = poly_conv_into(first, second, buf_a);
        let n = poly_conv_into(&eta, &buf_a[..m], buf_b);
        let mut acc = 0.0;
        for k in 0..n {
            acc = buf_b[k].mul_add(moments[k], acc);
        }
        acc
    };
    eta_second_term += conv_dot(
        second_coefficients_rs,
        first_coefficients_t,
        &mut buf_a,
        &mut buf_b,
    );
    eta_second_term += conv_dot(
        second_coefficients_rt,
        first_coefficients_s,
        &mut buf_a,
        &mut buf_b,
    );
    eta_second_term += conv_dot(
        second_coefficients_st,
        first_coefficients_r,
        &mut buf_a,
        &mut buf_b,
    );

    // cubic_coeff_term = Σ_{e,i,j,k} (eta·eta − 1)[e] · r[i] · s[j] · t[k] · moments[e+i+j+k].
    // Convolve r⊗s, then ⊗t, then ⊗(eta·eta − 1), giving a single dot.
    let mut eta_sq_minus_one = [0.0_f64; 7];
    for (i, &eta_i) in eta.iter().enumerate() {
        for (j, &eta_j) in eta.iter().enumerate() {
            eta_sq_minus_one[i + j] = eta_i.mul_add(eta_j, eta_sq_minus_one[i + j]);
        }
    }
    eta_sq_minus_one[0] -= 1.0;

    let rs_len = poly_conv_into(first_coefficients_r, first_coefficients_s, &mut buf_a);
    let rst_len = poly_conv_into(&buf_a[..rs_len], first_coefficients_t, &mut buf_b);
    // buf_a now reused for (eta_sq_minus_one ⊗ rst).
    let final_len = poly_conv_into(&eta_sq_minus_one, &buf_b[..rst_len], &mut buf_a);
    let mut cubic_coeff_term = 0.0;
    for k in 0..final_len {
        cubic_coeff_term = buf_a[k].mul_add(moments[k], cubic_coeff_term);
    }

    Ok((third_term - eta_second_term + cubic_coeff_term) * INV_TWO_PI)
}

#[inline]
pub fn cell_fourth_derivative_from_moments(
    cell: DenestedCubicCell,
    first_coefficients_r: &[f64],
    first_coefficients_s: &[f64],
    first_coefficients_t: &[f64],
    first_coefficients_u: &[f64],
    second_coefficients_rs: &[f64],
    second_coefficients_rt: &[f64],
    second_coefficients_ru: &[f64],
    second_coefficients_st: &[f64],
    second_coefficients_su: &[f64],
    second_coefficients_tu: &[f64],
    third_coefficients_rst: &[f64],
    third_coefficients_rsu: &[f64],
    third_coefficients_rtu: &[f64],
    third_coefficients_stu: &[f64],
    fourth_coefficients_rstu: &[f64],
    moments: &[f64],
) -> Result<f64, String> {
    let eta = [cell.c0, cell.c1, cell.c2, cell.c3];
    let r_degree = first_coefficients_degree("r", first_coefficients_r)?;
    let s_degree = first_coefficients_degree("s", first_coefficients_s)?;
    let t_degree = first_coefficients_degree("t", first_coefficients_t)?;
    let u_degree = first_coefficients_degree("u", first_coefficients_u)?;
    let linear_sum_degree = [
        third_coefficients_rst.len() + first_coefficients_u.len(),
        third_coefficients_rsu.len() + first_coefficients_t.len(),
        third_coefficients_rtu.len() + first_coefficients_s.len(),
        third_coefficients_stu.len() + first_coefficients_r.len(),
        second_coefficients_rs.len() + second_coefficients_tu.len(),
        second_coefficients_rt.len() + second_coefficients_su.len(),
        second_coefficients_ru.len() + second_coefficients_st.len(),
    ]
    .into_iter()
    .max()
    .unwrap_or(0)
    .saturating_sub(1);
    let quad_sum_degree = [
        second_coefficients_rs.len() + first_coefficients_t.len() + first_coefficients_u.len(),
        second_coefficients_rt.len() + first_coefficients_s.len() + first_coefficients_u.len(),
        second_coefficients_ru.len() + first_coefficients_s.len() + first_coefficients_t.len(),
        second_coefficients_st.len() + first_coefficients_r.len() + first_coefficients_u.len(),
        second_coefficients_su.len() + first_coefficients_r.len() + first_coefficients_t.len(),
        second_coefficients_tu.len() + first_coefficients_r.len() + first_coefficients_s.len(),
    ]
    .into_iter()
    .max()
    .unwrap_or(0)
    .saturating_sub(2);
    let quartic_product_degree = r_degree + s_degree + t_degree + u_degree;
    let needed = (fourth_coefficients_rstu.len().saturating_sub(1))
        .max(3 + linear_sum_degree)
        .max(6 + quad_sum_degree)
        .max(9 + quartic_product_degree);
    require_moments_degree(needed, moments, "fourth derivative")?;

    let fourth_term = moment_dot_with_coefficients_unchecked(fourth_coefficients_rstu, moments);

    // This is a deliberately serial leaf kernel: each call performs only a
    // handful of fixed-size polynomial convolutions, so Rayon fan-out belongs
    // at the surrounding row/cell batch level rather than inside this hot path.
    const SCRATCH: usize = 32;
    let max_linear_conv_len = [
        convolution_chain_len(&[
            eta.len(),
            third_coefficients_rst.len(),
            first_coefficients_u.len(),
        ]),
        convolution_chain_len(&[
            eta.len(),
            third_coefficients_rsu.len(),
            first_coefficients_t.len(),
        ]),
        convolution_chain_len(&[
            eta.len(),
            third_coefficients_rtu.len(),
            first_coefficients_s.len(),
        ]),
        convolution_chain_len(&[
            eta.len(),
            third_coefficients_stu.len(),
            first_coefficients_r.len(),
        ]),
        convolution_chain_len(&[
            eta.len(),
            second_coefficients_rs.len(),
            second_coefficients_tu.len(),
        ]),
        convolution_chain_len(&[
            eta.len(),
            second_coefficients_rt.len(),
            second_coefficients_su.len(),
        ]),
        convolution_chain_len(&[
            eta.len(),
            second_coefficients_ru.len(),
            second_coefficients_st.len(),
        ]),
    ]
    .into_iter()
    .max()
    .unwrap_or(0);
    let max_quad_conv_len = [
        convolution_chain_len(&[
            7,
            second_coefficients_rs.len(),
            first_coefficients_t.len(),
            first_coefficients_u.len(),
        ]),
        convolution_chain_len(&[
            7,
            second_coefficients_rt.len(),
            first_coefficients_s.len(),
            first_coefficients_u.len(),
        ]),
        convolution_chain_len(&[
            7,
            second_coefficients_ru.len(),
            first_coefficients_s.len(),
            first_coefficients_t.len(),
        ]),
        convolution_chain_len(&[
            7,
            second_coefficients_st.len(),
            first_coefficients_r.len(),
            first_coefficients_u.len(),
        ]),
        convolution_chain_len(&[
            7,
            second_coefficients_su.len(),
            first_coefficients_r.len(),
            first_coefficients_t.len(),
        ]),
        convolution_chain_len(&[
            7,
            second_coefficients_tu.len(),
            first_coefficients_r.len(),
            first_coefficients_s.len(),
        ]),
    ]
    .into_iter()
    .max()
    .unwrap_or(0);
    let max_quartic_conv_len = convolution_chain_len(&[
        10,
        first_coefficients_r.len(),
        first_coefficients_s.len(),
        first_coefficients_t.len(),
        first_coefficients_u.len(),
    ]);
    require_scratch_capacity(
        max_linear_conv_len
            .max(max_quad_conv_len)
            .max(max_quartic_conv_len),
        SCRATCH,
        "fourth derivative",
    )?;
    let mut buf_a = [0.0_f64; SCRATCH];
    let mut buf_b = [0.0_f64; SCRATCH];

    // eta_linear_term = Σ over seven (rst⊗u, rsu⊗t, rtu⊗s, stu⊗r, rs⊗tu,
    // rt⊗su, ru⊗st) of eta⊗product · moments. Fold each triple sum into
    // a single moment dot.
    let conv_eta_dot = |first: &[f64],
                        second: &[f64],
                        buf_a: &mut [f64; SCRATCH],
                        buf_b: &mut [f64; SCRATCH]|
     -> f64 {
        let m = poly_conv_into(first, second, buf_a);
        let n = poly_conv_into(&eta, &buf_a[..m], buf_b);
        let mut acc = 0.0;
        for k in 0..n {
            acc = buf_b[k].mul_add(moments[k], acc);
        }
        acc
    };
    let mut eta_linear_term = 0.0;
    eta_linear_term += conv_eta_dot(
        third_coefficients_rst,
        first_coefficients_u,
        &mut buf_a,
        &mut buf_b,
    );
    eta_linear_term += conv_eta_dot(
        third_coefficients_rsu,
        first_coefficients_t,
        &mut buf_a,
        &mut buf_b,
    );
    eta_linear_term += conv_eta_dot(
        third_coefficients_rtu,
        first_coefficients_s,
        &mut buf_a,
        &mut buf_b,
    );
    eta_linear_term += conv_eta_dot(
        third_coefficients_stu,
        first_coefficients_r,
        &mut buf_a,
        &mut buf_b,
    );
    eta_linear_term += conv_eta_dot(
        second_coefficients_rs,
        second_coefficients_tu,
        &mut buf_a,
        &mut buf_b,
    );
    eta_linear_term += conv_eta_dot(
        second_coefficients_rt,
        second_coefficients_su,
        &mut buf_a,
        &mut buf_b,
    );
    eta_linear_term += conv_eta_dot(
        second_coefficients_ru,
        second_coefficients_st,
        &mut buf_a,
        &mut buf_b,
    );

    let mut eta_sq_minus_one = [0.0_f64; 7];
    for (i, &eta_i) in eta.iter().enumerate() {
        for (j, &eta_j) in eta.iter().enumerate() {
            eta_sq_minus_one[i + j] = eta_i.mul_add(eta_j, eta_sq_minus_one[i + j]);
        }
    }
    eta_sq_minus_one[0] -= 1.0;

    // quad_coeff_term: six (eta²−1)⊗A⊗B⊗C · moments sums, where the (A,B,C)
    // factors are: (rs,t,u), (rt,s,u), (ru,s,t), (st,r,u), (su,r,t), (tu,r,s).
    let mut buf_c = [0.0_f64; SCRATCH];
    let conv_weighted_triple_dot = |weight: &[f64],
                                    a: &[f64],
                                    b: &[f64],
                                    c: &[f64],
                                    buf_a: &mut [f64; SCRATCH],
                                    buf_b: &mut [f64; SCRATCH],
                                    buf_c: &mut [f64; SCRATCH]|
     -> f64 {
        let ab_len = poly_conv_into(a, b, buf_a);
        let abc_len = poly_conv_into(&buf_a[..ab_len], c, buf_b);
        let final_len = poly_conv_into(weight, &buf_b[..abc_len], buf_c);
        let mut acc = 0.0;
        for k in 0..final_len {
            acc = buf_c[k].mul_add(moments[k], acc);
        }
        acc
    };
    let mut quad_coeff_term = 0.0;
    quad_coeff_term += conv_weighted_triple_dot(
        &eta_sq_minus_one,
        second_coefficients_rs,
        first_coefficients_t,
        first_coefficients_u,
        &mut buf_a,
        &mut buf_b,
        &mut buf_c,
    );
    quad_coeff_term += conv_weighted_triple_dot(
        &eta_sq_minus_one,
        second_coefficients_rt,
        first_coefficients_s,
        first_coefficients_u,
        &mut buf_a,
        &mut buf_b,
        &mut buf_c,
    );
    quad_coeff_term += conv_weighted_triple_dot(
        &eta_sq_minus_one,
        second_coefficients_ru,
        first_coefficients_s,
        first_coefficients_t,
        &mut buf_a,
        &mut buf_b,
        &mut buf_c,
    );
    quad_coeff_term += conv_weighted_triple_dot(
        &eta_sq_minus_one,
        second_coefficients_st,
        first_coefficients_r,
        first_coefficients_u,
        &mut buf_a,
        &mut buf_b,
        &mut buf_c,
    );
    quad_coeff_term += conv_weighted_triple_dot(
        &eta_sq_minus_one,
        second_coefficients_su,
        first_coefficients_r,
        first_coefficients_t,
        &mut buf_a,
        &mut buf_b,
        &mut buf_c,
    );
    quad_coeff_term += conv_weighted_triple_dot(
        &eta_sq_minus_one,
        second_coefficients_tu,
        first_coefficients_r,
        first_coefficients_s,
        &mut buf_a,
        &mut buf_b,
        &mut buf_c,
    );

    // cubic_weight = 3·eta − eta³ (same as the prior expansion: eta_sq*eta
    // negated, plus the 3·eta linear correction).
    let mut eta_sq = [0.0_f64; 7];
    for (i, &eta_i) in eta.iter().enumerate() {
        for (j, &eta_j) in eta.iter().enumerate() {
            eta_sq[i + j] = eta_i.mul_add(eta_j, eta_sq[i + j]);
        }
    }
    let mut cubic_weight = [0.0_f64; 10];
    for (i, &eta_sq_i) in eta_sq.iter().enumerate() {
        for (j, &eta_j) in eta.iter().enumerate() {
            cubic_weight[i + j] = (-eta_sq_i).mul_add(eta_j, cubic_weight[i + j]);
        }
    }
    for (idx, &eta_coeff) in eta.iter().enumerate() {
        cubic_weight[idx] += 3.0 * eta_coeff;
    }

    // quartic_coeff_term: cubic_weight ⊗ r ⊗ s ⊗ t ⊗ u · moments. The
    // original quintuple loop did 10·4·4·4·4 = 2560 mul-adds per call;
    // four sequential convolutions plus one moment dot drop this to
    // ~16+28+40+52+16 ≈ 152 mul-adds.
    let rs_len = poly_conv_into(first_coefficients_r, first_coefficients_s, &mut buf_a);
    let rst_len = poly_conv_into(&buf_a[..rs_len], first_coefficients_t, &mut buf_b);
    let rstu_len = poly_conv_into(&buf_b[..rst_len], first_coefficients_u, &mut buf_a);
    let final_len = poly_conv_into(&cubic_weight, &buf_a[..rstu_len], &mut buf_b);
    let mut quartic_coeff_term = 0.0;
    for k in 0..final_len {
        quartic_coeff_term = buf_b[k].mul_add(moments[k], quartic_coeff_term);
    }

    Ok((fourth_term - eta_linear_term + quad_coeff_term + quartic_coeff_term) * INV_TWO_PI)
}

#[inline]
pub fn global_cubic_from_local(span: LocalSpanCubic) -> (f64, f64, f64, f64) {
    let left = span.left;
    let q0 = span.c0 - span.c1 * left + span.c2 * left * left - span.c3 * left * left * left;
    let q1 = span.c1 - 2.0 * span.c2 * left + 3.0 * span.c3 * left * left;
    let q2 = span.c2 - 3.0 * span.c3 * left;
    let q3 = span.c3;
    (q0, q1, q2, q3)
}

/// Return the cubic polynomial coefficients (in `z`) of
/// `f(z) = link_span.evaluate(a + b*z)`.
///
/// `link_span.evaluate` is a cubic in its argument, so `f(z)` is also a cubic
/// in `z` and can be written exactly as
///
/// ```text
///     f(z) = d0 + d1·z + d2·z² + d3·z³
/// ```
///
/// where `(d0, d1, d2, d3)` are the values returned by this function. These
/// are **polynomial coefficients**, *not* derivatives of `f` at `z = 0`. The
/// relationship to Taylor derivatives is
///
/// ```text
///     d_k = f^(k)(0) / k!
/// ```
///
/// so `d0 = f(0)`, `d1 = f'(0)`, `d2 = ½·f''(0)`, `d3 = ⅙·f'''(0)`. Callers
/// such as [`denested_cell_coefficients`] and [`link_basis_cell_coefficients`]
/// rely on the polynomial-coefficient convention, since they propagate the
/// values directly as the `(c0, c1, c2, c3)` slots of a downstream polynomial
/// in `z`.
#[inline]
pub fn transformed_link_cubic(link_span: LocalSpanCubic, a: f64, b: f64) -> (f64, f64, f64, f64) {
    let shift = a - link_span.left;
    let d0 = link_span.c0
        + link_span.c1 * shift
        + link_span.c2 * shift * shift
        + link_span.c3 * shift * shift * shift;
    let d1 = b * (link_span.c1 + 2.0 * link_span.c2 * shift + 3.0 * link_span.c3 * shift * shift);
    let d2 = b * b * (link_span.c2 + 3.0 * link_span.c3 * shift);
    let d3 = link_span.c3 * b * b * b;
    (d0, d1, d2, d3)
}

#[inline]
pub fn denested_cell_coefficients(
    score_span: LocalSpanCubic,
    link_span: LocalSpanCubic,
    a: f64,
    b: f64,
) -> [f64; 4] {
    let (h0, h1, h2, h3) = global_cubic_from_local(score_span);
    let (d0, d1, d2, d3) = transformed_link_cubic(link_span, a, b);
    [a + b * h0 + d0, b + b * h1 + d1, b * h2 + d2, b * h3 + d3]
}

#[inline]
pub fn denested_cell_coefficient_partials(
    score_span: LocalSpanCubic,
    link_span: LocalSpanCubic,
    a: f64,
    b: f64,
) -> ([f64; 4], [f64; 4]) {
    let (h0, h1, h2, h3) = global_cubic_from_local(score_span);
    let shift = a - link_span.left;
    let alpha1 = link_span.c1;
    let alpha2 = link_span.c2;
    let alpha3 = link_span.c3;
    let dc_da = [
        1.0 + alpha1 + 2.0 * alpha2 * shift + 3.0 * alpha3 * shift * shift,
        b * (2.0 * alpha2 + 6.0 * alpha3 * shift),
        3.0 * alpha3 * b * b,
        0.0,
    ];
    let dc_db = [
        h0,
        1.0 + h1 + alpha1 + 2.0 * alpha2 * shift + 3.0 * alpha3 * shift * shift,
        h2 + 2.0 * b * (alpha2 + 3.0 * alpha3 * shift),
        h3 + 3.0 * alpha3 * b * b,
    ];
    (dc_da, dc_db)
}

#[inline]
fn link_cubic_second_partials(
    link_span: LocalSpanCubic,
    a: f64,
    b: f64,
) -> ([f64; 4], [f64; 4], [f64; 4]) {
    let shift = a - link_span.left;
    let alpha2 = link_span.c2;
    let alpha3 = link_span.c3;
    let dc_daa = [
        2.0 * alpha2 + 6.0 * alpha3 * shift,
        6.0 * alpha3 * b,
        0.0,
        0.0,
    ];
    let dc_dab = [
        0.0,
        2.0 * alpha2 + 6.0 * alpha3 * shift,
        6.0 * alpha3 * b,
        0.0,
    ];
    let dc_dbb = [
        0.0,
        0.0,
        2.0 * (alpha2 + 3.0 * alpha3 * shift),
        6.0 * alpha3 * b,
    ];
    (dc_daa, dc_dab, dc_dbb)
}

#[inline]
pub fn denested_cell_second_partials(
    score_span: LocalSpanCubic,
    link_span: LocalSpanCubic,
    a: f64,
    b: f64,
) -> ([f64; 4], [f64; 4], [f64; 4]) {
    let score_left = score_span.left;
    if !score_left.is_finite() {
        return ([f64::NAN; 4], [f64::NAN; 4], [f64::NAN; 4]);
    }
    link_cubic_second_partials(link_span, a, b)
}

#[inline]
fn link_cubic_third_partials(
    link_span: LocalSpanCubic,
) -> ([f64; 4], [f64; 4], [f64; 4], [f64; 4]) {
    let alpha3 = link_span.c3;
    (
        [6.0 * alpha3, 0.0, 0.0, 0.0],
        [0.0, 6.0 * alpha3, 0.0, 0.0],
        [0.0, 0.0, 6.0 * alpha3, 0.0],
        [0.0, 0.0, 0.0, 6.0 * alpha3],
    )
}

#[inline]
pub fn denested_cell_third_partials(
    link_span: LocalSpanCubic,
) -> ([f64; 4], [f64; 4], [f64; 4], [f64; 4]) {
    link_cubic_third_partials(link_span)
}

#[inline]
pub fn score_basis_cell_coefficients(score_basis_span: LocalSpanCubic, b: f64) -> [f64; 4] {
    let (h0, h1, h2, h3) = global_cubic_from_local(score_basis_span);
    [b * h0, b * h1, b * h2, b * h3]
}

#[inline]
pub fn link_basis_cell_coefficients(link_basis_span: LocalSpanCubic, a: f64, b: f64) -> [f64; 4] {
    let (d0, d1, d2, d3) = transformed_link_cubic(link_basis_span, a, b);
    [d0, d1, d2, d3]
}

#[inline]
pub fn link_basis_cell_coefficient_partials(
    link_basis_span: LocalSpanCubic,
    a: f64,
    b: f64,
) -> ([f64; 4], [f64; 4]) {
    let shift = a - link_basis_span.left;
    let alpha1 = link_basis_span.c1;
    let alpha2 = link_basis_span.c2;
    let alpha3 = link_basis_span.c3;
    let dc_da = [
        alpha1 + 2.0 * alpha2 * shift + 3.0 * alpha3 * shift * shift,
        b * (2.0 * alpha2 + 6.0 * alpha3 * shift),
        3.0 * alpha3 * b * b,
        0.0,
    ];
    let dc_db = [
        0.0,
        alpha1 + 2.0 * alpha2 * shift + 3.0 * alpha3 * shift * shift,
        2.0 * b * (alpha2 + 3.0 * alpha3 * shift),
        3.0 * alpha3 * b * b,
    ];
    (dc_da, dc_db)
}

#[inline]
pub fn link_basis_cell_second_partials(
    link_basis_span: LocalSpanCubic,
    a: f64,
    b: f64,
) -> ([f64; 4], [f64; 4], [f64; 4]) {
    link_cubic_second_partials(link_basis_span, a, b)
}

#[inline]
pub fn link_basis_cell_third_partials(
    link_basis_span: LocalSpanCubic,
) -> ([f64; 4], [f64; 4], [f64; 4], [f64; 4]) {
    link_cubic_third_partials(link_basis_span)
}

pub fn build_denested_partition_cells<FS, FL>(
    a: f64,
    b: f64,
    score_breaks: &[f64],
    link_breaks: &[f64],
    score_span_at: FS,
    link_span_at: FL,
) -> Result<Vec<DenestedPartitionCell>, String>
where
    FS: FnMut(f64) -> Result<LocalSpanCubic, String>,
    FL: FnMut(f64) -> Result<LocalSpanCubic, String>,
{
    build_denested_partition_cells_with_tails(
        a,
        b,
        score_breaks,
        link_breaks,
        score_span_at,
        link_span_at,
    )
}

/// Build a partition covering `(-∞, +∞)` with parameter-independent outer
/// bounds.  Interior cells use the same finite-cell polynomial algebra.
/// The two tail cells are guaranteed affine (c2=c3=0) because both
/// deviations saturate to constants outside their knot support.
///
/// The tail cells' score/link spans come from the same closures evaluated
/// at a representative point in the tail region — the closures must return
/// constant (c1=c2=c3=0) cubics for points outside support.
pub fn build_denested_partition_cells_with_tails<FS, FL>(
    a: f64,
    b: f64,
    score_breaks: &[f64],
    link_breaks: &[f64],
    mut score_span_at: FS,
    mut link_span_at: FL,
) -> Result<Vec<DenestedPartitionCell>, String>
where
    FS: FnMut(f64) -> Result<LocalSpanCubic, String>,
    FL: FnMut(f64) -> Result<LocalSpanCubic, String>,
{
    // Collect all INTERNAL split points (finite), each tagged with its
    // provenance: a fixed score break or a link-knot crossing. Provenance
    // identifies the cell's `(a, b)` family for the Chebyshev moment-family
    // layer; the z coordinates alone cannot distinguish the two kinds.
    let mut split_points: Vec<(f64, PartitionEdge)> = score_breaks
        .iter()
        .map(|&sigma| (sigma, PartitionEdge::Fixed(sigma)))
        .collect();
    if b.abs() > 1e-12 {
        for &tau in link_breaks {
            let z = (tau - a) / b;
            if z.is_finite() {
                split_points.push((z, PartitionEdge::Crossing { tau }));
            }
        }
    }
    dedup_sorted_tagged_breakpoints(&mut split_points);

    let mut out = Vec::new();

    if split_points.is_empty() {
        let score_span = score_span_at(0.0)?;
        let link_span = link_span_at(a)?;
        let coeffs = denested_cell_coefficients(score_span, link_span, a, b);
        return Ok(vec![DenestedPartitionCell {
            cell: DenestedCubicCell {
                left: f64::NEG_INFINITY,
                right: f64::INFINITY,
                c0: coeffs[0],
                c1: coeffs[1],
                c2: 0.0,
                c3: 0.0,
            },
            score_span,
            link_span,
            left_edge: PartitionEdge::Fixed(f64::NEG_INFINITY),
            right_edge: PartitionEdge::Fixed(f64::INFINITY),
        }]);
    }

    // ── Left tail cell: (-∞, leftmost_split] ──
    let (leftmost, leftmost_edge) = split_points[0];
    // Evaluate spans at a point just left of the leftmost split.  The
    // closures return constant tail cubics for this region.
    let left_probe = interval_probe_point(f64::NEG_INFINITY, leftmost)?;
    let left_score_span = score_span_at(left_probe)?;
    let left_link_span = link_span_at(a + b * left_probe)?;
    let left_coeffs = denested_cell_coefficients(left_score_span, left_link_span, a, b);
    if left_coeffs[2].abs() > NORMALIZED_CELL_BRANCH_TOL
        || left_coeffs[3].abs() > NORMALIZED_CELL_BRANCH_TOL
    {
        return Err(CubicCellKernelError::invalid_cell_shape(format!(
            "left tail cell must be affine (deviations constant outside support), \
             got c2={:.3e}, c3={:.3e}",
            left_coeffs[2], left_coeffs[3]
        ))
        .into());
    }
    out.push(DenestedPartitionCell {
        cell: DenestedCubicCell {
            left: f64::NEG_INFINITY,
            right: leftmost,
            c0: left_coeffs[0],
            c1: left_coeffs[1],
            c2: 0.0,
            c3: 0.0,
        },
        score_span: left_score_span,
        link_span: left_link_span,
        left_edge: PartitionEdge::Fixed(f64::NEG_INFINITY),
        right_edge: leftmost_edge,
    });

    // ── Interior cells (all finite) ──
    for window in split_points.windows(2) {
        let (left, left_edge) = window[0];
        let (right, right_edge) = window[1];
        if !left.is_finite() || !right.is_finite() || right - left <= 1e-12 {
            continue;
        }
        let mid = interval_probe_point(left, right)?;
        let score_span = score_span_at(mid)?;
        let link_span = link_span_at(a + b * mid)?;
        let coeffs = denested_cell_coefficients(score_span, link_span, a, b);
        out.push(DenestedPartitionCell {
            cell: DenestedCubicCell {
                left,
                right,
                c0: coeffs[0],
                c1: coeffs[1],
                c2: coeffs[2],
                c3: coeffs[3],
            },
            score_span,
            link_span,
            left_edge,
            right_edge,
        });
    }

    // ── Right tail cell: [rightmost_split, +∞) ──
    let (rightmost, rightmost_edge) = *split_points.last().unwrap();
    let right_probe = interval_probe_point(rightmost, f64::INFINITY)?;
    let right_score_span = score_span_at(right_probe)?;
    let right_link_span = link_span_at(a + b * right_probe)?;
    let right_coeffs = denested_cell_coefficients(right_score_span, right_link_span, a, b);
    if right_coeffs[2].abs() > NORMALIZED_CELL_BRANCH_TOL
        || right_coeffs[3].abs() > NORMALIZED_CELL_BRANCH_TOL
    {
        return Err(CubicCellKernelError::invalid_cell_shape(format!(
            "right tail cell must be affine (deviations constant outside support), \
             got c2={:.3e}, c3={:.3e}",
            right_coeffs[2], right_coeffs[3]
        ))
        .into());
    }
    out.push(DenestedPartitionCell {
        cell: DenestedCubicCell {
            left: rightmost,
            right: f64::INFINITY,
            c0: right_coeffs[0],
            c1: right_coeffs[1],
            c2: 0.0,
            c3: 0.0,
        },
        score_span: right_score_span,
        link_span: right_link_span,
        left_edge: rightmost_edge,
        right_edge: PartitionEdge::Fixed(f64::INFINITY),
    });

    Ok(out)
}

#[inline]
pub fn normalized_non_affine_coefficients(
    left: f64,
    right: f64,
    c0: f64,
    c1: f64,
    c2: f64,
    c3: f64,
) -> Result<(f64, f64), String> {
    let width = right - left;
    if !width.is_finite() || width <= 0.0 {
        return Err(CubicCellKernelError::invalid_cell_shape(format!(
            "normalized cubic coefficients require a positive finite cell width, got left={left}, right={right}"
        ))
        .into());
    }
    let anchor_scale = c0.abs() + c1.abs();
    if !anchor_scale.is_finite() {
        return Err(CubicCellKernelError::invalid_cell_shape(format!(
            "normalized cubic coefficients require finite affine coefficients, got c0={c0}, c1={c1}"
        ))
        .into());
    }
    let mid = 0.5 * (left + right);
    let half = 0.5 * width;
    let k2 = half * half * (c2 + 3.0 * c3 * mid);
    let k3 = c3 * half * half * half;
    Ok((k2, k3))
}

#[inline]
pub fn branch_cell(cell: DenestedCubicCell) -> Result<ExactCellBranch, String> {
    let tol = effective_branch_tol(cell);
    if !cell.left.is_finite() || !cell.right.is_finite() {
        if cell.c2.abs() <= tol && cell.c3.abs() <= tol {
            return Ok(ExactCellBranch::Affine);
        }
        return Err(CubicCellKernelError::invalid_cell_shape(format!(
            "non-affine cells require finite bounds, got [{}, {}] with c2={:.6e}, c3={:.6e}",
            cell.left, cell.right, cell.c2, cell.c3
        ))
        .into());
    }
    let (k2, k3) = normalized_non_affine_coefficients(
        cell.left, cell.right, cell.c0, cell.c1, cell.c2, cell.c3,
    )?;
    if k2.abs() <= tol && k3.abs() <= tol {
        Ok(ExactCellBranch::Affine)
    } else if k3.abs() <= tol {
        Ok(ExactCellBranch::Quartic)
    } else {
        Ok(ExactCellBranch::Sextic)
    }
}

#[inline]
fn degenerate_sextic_branch(
    cell: DenestedCubicCell,
    lead: f64,
) -> Result<Option<ExactCellBranch>, String> {
    // The sextic recurrence divides by `lead = 3*c3^2`. When that division is
    // unstable, lower the polynomial degree without discarding a material
    // quadratic coefficient.
    let (normalized_k2, normalized_k3) = normalized_non_affine_coefficients(
        cell.left, cell.right, cell.c0, cell.c1, cell.c2, cell.c3,
    )?;
    if normalized_k3.abs() > NORMALIZED_CELL_BRANCH_TOL && lead.abs() > 1e-18 {
        return Ok(None);
    }
    if normalized_k2.abs() > NORMALIZED_CELL_BRANCH_TOL {
        Ok(Some(ExactCellBranch::Quartic))
    } else {
        Ok(Some(ExactCellBranch::Affine))
    }
}

#[inline]
fn validate_bvn_args(h: f64, k: f64, rho: f64) -> Result<(), String> {
    if !h.is_finite() && !h.is_infinite() {
        return Err(CubicCellKernelError::bivariate_normal_domain(
            "bivariate normal cdf requires finite or infinite h",
        )
        .into());
    }
    if !k.is_finite() && !k.is_infinite() {
        return Err(CubicCellKernelError::bivariate_normal_domain(
            "bivariate normal cdf requires finite or infinite k",
        )
        .into());
    }
    if !rho.is_finite() {
        return Err(CubicCellKernelError::bivariate_normal_domain(format!(
            "bivariate normal cdf requires finite correlation, got {rho}"
        ))
        .into());
    }
    Ok::<(), _>(())
}

#[inline]
fn bvn_gl_sum(h: f64, k: f64, rho_clamped: f64, asr: f64) -> f64 {
    // The Drezner-Wesolowsky arcsin representation is integrated with the
    // same 20-point Gauss-Legendre rule as before, but mirrored node pairs are
    // evaluated with one sin_cos for the half-angle offset rather than two
    // independent sin calls.  This preserves the quadrature rule (and hence
    // the accuracy envelope) while reducing the transcendental work in the
    // dominant finite-bound path from 20 sin calls to 11 sin/cos evaluations.
    if rho_clamped == 0.0 {
        return 0.0;
    }
    let hs = 0.5 * (h * h + k * k);
    let hk = h * k;
    let half_asr = 0.5 * asr;
    let (sin_mid, cos_mid) = half_asr.sin_cos();
    let mut sum = 0.0;
    for i in 0..10 {
        let node = GL20_NODES[i].abs();
        let weight = GL20_WEIGHTS[i];
        let (sin_delta, cos_delta) = (half_asr * node).sin_cos();

        let sn_lo = sin_mid * cos_delta - cos_mid * sin_delta;
        let one_minus_lo = 1.0 - sn_lo * sn_lo;
        let expo_lo = ((sn_lo * hk) - hs) / one_minus_lo;

        let sn_hi = sin_mid * cos_delta + cos_mid * sin_delta;
        let one_minus_hi = 1.0 - sn_hi * sn_hi;
        let expo_hi = ((sn_hi * hk) - hs) / one_minus_hi;

        sum += weight * (expo_lo.exp() + expo_hi.exp());
    }
    sum
}

pub fn bivariate_normal_cdf(h: f64, k: f64, rho: f64) -> Result<f64, String> {
    validate_bvn_args(h, k, rho)?;
    if h == f64::NEG_INFINITY || k == f64::NEG_INFINITY {
        return Ok(0.0);
    }
    if h == f64::INFINITY {
        return Ok(normal_cdf(k));
    }
    if k == f64::INFINITY {
        return Ok(normal_cdf(h));
    }

    let rho_clamped = rho.clamp(-1.0, 1.0);
    if rho_clamped >= 1.0 - 1e-12 {
        return Ok(normal_cdf(h.min(k)));
    }
    if rho_clamped <= -1.0 + 1e-12 {
        return Ok((normal_cdf(h) - normal_cdf(-k)).clamp(0.0, 1.0));
    }
    if rho_clamped == 0.0 {
        return Ok((normal_cdf(h) * normal_cdf(k)).clamp(0.0, 1.0));
    }
    if h == 0.0 && k == 0.0 {
        return Ok((0.25 + rho_clamped.asin() / std::f64::consts::TAU).clamp(0.0, 1.0));
    }

    let asr = rho_clamped.asin();
    let sum = bvn_gl_sum(h, k, rho_clamped, asr);
    Ok((normal_cdf(h) * normal_cdf(k) + asr * sum / (4.0 * std::f64::consts::PI)).clamp(0.0, 1.0))
}

#[inline]
fn bvn_gl_sum_interval(h: f64, left: f64, right: f64, rho_clamped: f64, asr: f64) -> f64 {
    if rho_clamped == 0.0 {
        return 0.0;
    }
    let h2 = h * h;
    let right_hs = 0.5 * (h2 + right * right);
    let left_hs = 0.5 * (h2 + left * left);
    let half_asr = 0.5 * asr;
    let (sin_mid, cos_mid) = half_asr.sin_cos();
    let mut sum = 0.0;
    for i in 0..10 {
        let node = GL20_NODES[i].abs();
        let weight = GL20_WEIGHTS[i];
        let (sin_delta, cos_delta) = (half_asr * node).sin_cos();

        let sn_lo = sin_mid * cos_delta - cos_mid * sin_delta;
        let one_minus_lo = 1.0 - sn_lo * sn_lo;
        let lo_right = (((sn_lo * h * right) - right_hs) / one_minus_lo).exp();
        let lo_left = (((sn_lo * h * left) - left_hs) / one_minus_lo).exp();

        let sn_hi = sin_mid * cos_delta + cos_mid * sin_delta;
        let one_minus_hi = 1.0 - sn_hi * sn_hi;
        let hi_right = (((sn_hi * h * right) - right_hs) / one_minus_hi).exp();
        let hi_left = (((sn_hi * h * left) - left_hs) / one_minus_hi).exp();

        sum += weight * ((lo_right - lo_left) + (hi_right - hi_left));
    }
    sum
}

fn bivariate_normal_cdf_interval(h: f64, left: f64, right: f64, rho: f64) -> Result<f64, String> {
    if right <= left {
        return Ok(0.0);
    }
    if left == f64::NEG_INFINITY && right == f64::INFINITY {
        return Ok(normal_cdf(h));
    }
    if !left.is_finite() || !right.is_finite() {
        let upper = bivariate_normal_cdf(h, right, rho)?;
        let lower = bivariate_normal_cdf(h, left, rho)?;
        return Ok((upper - lower).clamp(0.0, 1.0));
    }
    validate_bvn_args(h, left, rho)?;
    validate_bvn_args(h, right, rho)?;
    if h == f64::NEG_INFINITY {
        return Ok(0.0);
    }
    if h == f64::INFINITY {
        return Ok((normal_cdf(right) - normal_cdf(left)).clamp(0.0, 1.0));
    }

    let rho_clamped = rho.clamp(-1.0, 1.0);
    if rho_clamped >= 1.0 - 1e-12 || rho_clamped <= -1.0 + 1e-12 {
        let upper = bivariate_normal_cdf(h, right, rho_clamped)?;
        let lower = bivariate_normal_cdf(h, left, rho_clamped)?;
        return Ok((upper - lower).clamp(0.0, 1.0));
    }

    let cdf_h = normal_cdf(h);
    let normal_part = cdf_h * (normal_cdf(right) - normal_cdf(left));
    if rho_clamped == 0.0 {
        return Ok(normal_part.clamp(0.0, 1.0));
    }
    let asr = rho_clamped.asin();
    let sum = bvn_gl_sum_interval(h, left, right, rho_clamped, asr);
    Ok((normal_part + asr * sum / (4.0 * std::f64::consts::PI)).clamp(0.0, 1.0))
}

fn exp_neg_half_square(x: f64) -> f64 {
    if x.is_infinite() {
        0.0
    } else {
        (-0.5 * x * x).exp()
    }
}

/// Zeroth truncated standard-normal moment `T_0(a, b) = ∫_a^b e^(−z²/2) dz
/// = √(2π)·(Φ(b) − Φ(a))`, evaluated without catastrophic cancellation in
/// either tail.
///
/// Writing `T_0 = √(π/2)·[erf(b/√2) − erf(a/√2)]`, the naive form collapses
/// to `0.0` whenever both endpoints lie in the *same* far tail: `erf`
/// saturates at the IEEE-754 values `±1.0` for `|x| ≳ 8.3·√2`, so the
/// difference of two saturated values is exactly zero even though the
/// integral is a strictly positive number well inside the f64 normal range
/// (e.g. `∫_{-12}^{-10} ≈ 1.9e-23`). The fix is to reduce the erf difference
/// to complementary tail probabilities — `erfc` is evaluated with a dedicated
/// tail series, *not* as `1 − erf` — and to pick, by the sign of the
/// endpoints, the algebraically-equivalent form whose terms do not cancel
/// against one another:
///
/// ```text
/// both ≥ 0 (upper tail):  erf(b/√2) − erf(a/√2) = erfc(a/√2) − erfc(b/√2)
/// both ≤ 0 (lower tail):  erf(b/√2) − erf(a/√2) = erfc(−b/√2) − erfc(−a/√2)
/// straddling zero:        erf(b/√2) − erf(a/√2)
///                        = erf(b/√2) + erf(−a/√2)       near the anchor
///                        = 2 − erfc(b/√2) − erfc(−a/√2) otherwise
/// ```
///
/// In each branch every `erfc` argument is `≥ 0`, so the terms are small
/// positive tail values, while narrow straddling intervals add two
/// non-negative `erf` masses measured outward from the anchor. That avoids
/// the `2 − erfc(b/√2) − erfc(−a/√2)` cancellation when both erfc terms round
/// to `1.0`, but keeps the erfc-tail form for ordinary/full-line straddling
/// intervals. No large quantities cancel and full f64 precision survives down
/// to the underflow boundary in either tail and around the affine anchor.
///
/// Uses `libm::erfc` (msun double-precision implementation, ≤ 1 ulp) rather
/// than `statrs::function::erf::erfc` (a 6-term rational approximation that
/// carries ~3·10⁻¹¹ relative error around `|x| ≈ 1/√2` — see the existing
/// `libm::erfc` consumer at `inference::polya_gamma_core::normal_cdf`). That
/// statrs error propagates directly into `T_0`, then through every higher
/// moment `T_n` (the recurrence `T_n = a^{n-1}e^{-a²/2} − b^{n-1}e^{-b²/2}
/// + (n-1)·T_{n-2}` walks `T_0` up two steps at a time), then through every
/// affine-cell moment via `affine_anchor_moment_vector` (whose `out[n]` is a
/// linear combination of `T_0..=T_n`), and is the dominant source of error
/// in the affine-cell branch of the cubic-cell substrate (CPU/GPU parity
/// reference for transformation-normal, bernoulli-marginal-slope, and the
/// BMS flex-row higher-derivative reuse path).
fn truncated_gaussian_zeroth_moment(a: f64, b: f64) -> f64 {
    let inv_sqrt2 = 1.0 / std::f64::consts::SQRT_2;
    let za = a * inv_sqrt2;
    let zb = b * inv_sqrt2;
    let erf_diff = if za >= 0.0 {
        libm::erfc(za) - libm::erfc(zb)
    } else if zb <= 0.0 {
        libm::erfc(-zb) - libm::erfc(-za)
    } else if zb <= 0.5 && -za <= 0.5 {
        // Near the affine anchor, erfc(zb) and erfc(-za) are both close to
        // one; subtracting them from 2.0 can round a tiny but representable
        // cell mass to zero. The equivalent erf sum adds small positive
        // quantities directly.
        libm::erf(zb) + libm::erf(-za)
    } else {
        2.0 - libm::erfc(zb) - libm::erfc(-za)
    };
    // √(2π)·½ = √(π/2).
    (std::f64::consts::PI / 2.0).sqrt() * erf_diff
}

/// Fill `out[0..=max_degree]` with the raw truncated standard-normal moments
///
/// ```text
/// T_n(a, b) = ∫_a^b z^n exp(-z²/2) dz
/// ```
///
/// using the integration-by-parts recurrence
///
/// ```text
/// T_0(a, b) = √(2π) (Φ(b) − Φ(a))
/// T_1(a, b) = exp(−a²/2) − exp(−b²/2)
/// T_n(a, b) = a^(n−1) e^{−a²/2} − b^(n−1) e^{−b²/2} + (n−1) T_{n−2}(a, b)
/// ```
///
/// Computed in one forward sweep so each call evaluates `erf` and
/// `exp(−x²/2)` exactly twice (once at `a`, once at `b`) regardless of the
/// requested degree. The naive form — calling `T_n` recursively for each
/// `n = 0..=max_degree` — re-evaluated `erf`/`exp` about `max_degree²/4`
/// times per affine cell, which dominated the wall time of the
/// transformation-normal and bernoulli-marginal-slope inner solves with
/// `max_degree = 64` (the transport order's required degree budget).
fn fill_truncated_gaussian_moments(a: f64, b: f64, out: &mut [f64]) {
    if out.is_empty() {
        return;
    }
    out[0] = truncated_gaussian_zeroth_moment(a, b);
    if out.len() == 1 {
        return;
    }
    let ea = exp_neg_half_square(a);
    let eb = exp_neg_half_square(b);
    out[1] = ea - eb;
    if out.len() == 2 {
        return;
    }
    let a_finite = a.is_finite();
    let b_finite = b.is_finite();
    // For n in 2..=max_degree we need a^{n-1} e^{-a²/2} (resp. b). Carry the
    // running powers a^{n-1}, b^{n-1} forward by a single multiply per step.
    // Infinite endpoints contribute 0 (the integrand decays at the rate of
    // exp(−x²/2)), matching the prior `is_infinite` branch in the recursive
    // implementation; we still update the running power so the iteration
    // stays branchless when both endpoints are finite.
    let mut a_pow_n_minus_1 = a; // a^1, used at n = 2
    let mut b_pow_n_minus_1 = b;
    for n in 2..out.len() {
        let left = if a_finite { a_pow_n_minus_1 * ea } else { 0.0 };
        let right = if b_finite { b_pow_n_minus_1 * eb } else { 0.0 };
        out[n] = left - right + (n as f64 - 1.0) * out[n - 2];
        a_pow_n_minus_1 *= a;
        b_pow_n_minus_1 *= b;
    }
}

/// Stack-array bound for `affine_anchor_moment_vector_into`. Public callers
/// use up to ~24 (largest is the bernoulli-margslope outer-step degree-21
/// reduction); 64 leaves comfortable headroom without growing the per-call
/// stack footprint meaningfully.
const MAX_AFFINE_ANCHOR_DEGREE: usize = 64;

pub fn affine_anchor_moment_vector(
    alpha: f64,
    beta: f64,
    left: f64,
    right: f64,
    max_degree: usize,
) -> Vec<f64> {
    let mut out = vec![0.0; max_degree + 1];
    affine_anchor_moment_vector_into(alpha, beta, left, right, max_degree, &mut out);
    out
}

fn affine_anchor_moment_vector_into(
    alpha: f64,
    beta: f64,
    left: f64,
    right: f64,
    max_degree: usize,
    out: &mut [f64],
) {
    assert_eq!(out.len(), max_degree + 1);
    let s = (1.0 + beta * beta).sqrt();
    let mu = -alpha * beta / (1.0 + beta * beta);
    let y_left = if left.is_infinite() {
        if left.is_sign_positive() {
            f64::INFINITY
        } else {
            f64::NEG_INFINITY
        }
    } else {
        s * (left - mu)
    };
    let y_right = if right.is_infinite() {
        if right.is_sign_positive() {
            f64::INFINITY
        } else {
            f64::NEG_INFINITY
        }
    } else {
        s * (right - mu)
    };
    let anchor = (-alpha * alpha / (2.0 * s * s)).exp() / s;
    assert!(
        max_degree <= MAX_AFFINE_ANCHOR_DEGREE,
        "affine_anchor_moment_vector max_degree {} exceeds compile-time bound {}",
        max_degree,
        MAX_AFFINE_ANCHOR_DEGREE
    );
    let mut t = [0.0_f64; MAX_AFFINE_ANCHOR_DEGREE + 1];
    fill_truncated_gaussian_moments(y_left, y_right, &mut t[..=max_degree]);
    // Build mu^k and s^{-k} tables once. The inner sum is the binomial
    // expansion of the affine change-of-variables, and computing the
    // binomial coefficient via Pascal's row recurrence + carrying mu/s
    // powers eliminates the per-(n, k) `powi` and binomial calls that
    // otherwise dominated the inner loop at large `max_degree`.
    let mut mu_pow = [1.0_f64; MAX_AFFINE_ANCHOR_DEGREE + 1];
    for k in 1..=max_degree {
        mu_pow[k] = mu_pow[k - 1] * mu;
    }
    let inv_s = 1.0 / s;
    let mut inv_s_pow = [1.0_f64; MAX_AFFINE_ANCHOR_DEGREE + 1];
    for k in 1..=max_degree {
        inv_s_pow[k] = inv_s_pow[k - 1] * inv_s;
    }
    out.fill(0.0);
    for n in 0..=max_degree {
        let mut acc = 0.0;
        // C(n, k+1) = C(n, k) · (n − k) / (k + 1).
        let mut binom = 1.0;
        for k in 0..=n {
            let term = binom * mu_pow[n - k] * inv_s_pow[k];
            acc = term.mul_add(t[k], acc);
            if k < n {
                binom = binom * (n - k) as f64 / (k + 1) as f64;
            }
        }
        out[n] = anchor * acc;
    }
}

fn affine_value_from_moment_primitive(alpha: f64, beta: f64, left: f64, right: f64) -> f64 {
    // Exact formula via bivariate normal CDF.
    //
    // V(α,β,l,r) = ∫_l^r Φ(α+βz)φ(z)dz
    //            = P(U ≤ α+βZ, l ≤ Z ≤ r)    where U,Z iid N(0,1)
    //            = Φ₂(h, r; ρ) − Φ₂(h, l; ρ)
    //
    // with h = α/√(1+β²) and ρ = −β/√(1+β²).
    //
    // This is exact to floating-point precision via the high-accuracy
    // Drezner-Wesolowsky BVN routine, replacing the previous fixed 20-point
    // Gauss-Legendre numerical integration of the derivative primitive.
    let s = (1.0 + beta * beta).sqrt();
    let h = alpha / s;
    let rho = -beta / s;
    bivariate_normal_cdf_interval(h, left, right, rho).unwrap_or(0.0)
}

/// Evaluate an affine cell (c2=c3=0) with a value/moment-consistent primitive.
///
/// Value and moments are now generated from the same affine moment primitive.
/// The zero-moment derivative is exact, and `value` is reconstructed by
/// integrating `d value / d alpha = INV_TWO_PI * moments[0]` over `alpha`
/// on a transformed semi-infinite domain.
pub fn evaluate_affine_cell_state(
    cell: DenestedCubicCell,
    max_degree: usize,
) -> Result<CellMomentState, String> {
    let alpha = cell.c0;
    let beta = cell.c1;
    let value = affine_value_from_moment_primitive(alpha, beta, cell.left, cell.right);
    let moments = affine_anchor_moment_vector(alpha, beta, cell.left, cell.right, max_degree);
    Ok(CellMomentState {
        branch: ExactCellBranch::Affine,
        value,
        moments: moments.into(),
    })
}

fn evaluate_affine_cell_derivative_state(
    cell: DenestedCubicCell,
    max_degree: usize,
) -> Result<CellDerivativeMomentState, String> {
    let alpha = cell.c0;
    let beta = cell.c1;
    let moments = affine_anchor_moment_vector(alpha, beta, cell.left, cell.right, max_degree);
    Ok(CellDerivativeMomentState {
        branch: ExactCellBranch::Affine,
        moments: moments.into(),
    })
}

/// Accumulate `mw * z^k` into `moments[k]` for k=0..moments.len(). The
/// "unrolled4" name is historical — this is the plain scalar accumulator
/// that the SIMD outer loop calls per lane. Moment counts are small enough
/// (max_degree + 1 <= ~10) that explicit 4-way unrolling does not measurably
/// improve throughput over the iterator path; the wide::f64x4::exp savings
/// in the SIMD outer dominate the kernel's runtime.
#[inline]
fn accumulate_moments_unrolled4(moments: &mut [f64], mw: f64, z: f64) {
    let mut z_pow = 1.0_f64;
    for slot in moments.iter_mut() {
        *slot = mw.mul_add(z_pow, *slot);
        z_pow *= z;
    }
}

// Shared SIMD Gauss-Legendre core for non-affine cells. The const generic
// `COMPUTE_VALUE` selects whether the cell value integral
// `∫ φ(η(z)) · exp(-½z²) dz / √(2π)` is accumulated alongside the moments.
// Monomorphization collapses the const-generic branches at compile time, so
// `COMPUTE_VALUE = false` emits the moment-only path verbatim.
//
// Single source of truth for the moment SIMD lane ordering, the Horner-with-FMA
// pattern for η(z), the `0.5 * (z² + η²)` quadratic-form evaluation order, the
// unscaled per-node GL moment weights, the post-loop half-width fold, and the
// per-lane `accumulate_moments_unrolled4` call. The previous duplicated code paths
// drifted by 1 ULP whenever any of these details diverged; here both paths
// share the same instructions, eliminating an entire class of regressions
// where a tweak to the quadrature order or the FMA pattern would silently
// re-introduce divergence between the value- and derivative-only callers.
//
// Gauss-Legendre on [left, right] converges geometrically for the analytic
// integrand exp(-q(z)) with quartic/sextic q on a bounded cell; the prior
// adaptive transport path expanded basis_moments via the forward 3-/5-step
// recurrences in reduce_quartic/sextic_moments, which amplify roundoff by
// (1/lead)^n with lead = 2c2²/3c3² and overflow to NaN for small c2/c3 cells
// that arise naturally in production.
//
// The fixed 384-node rule that replaced the transport path is accurate but
// pays ~384 exp evaluations per cell unconditionally. Production cells are
// narrow spline-knot subdivisions where a 12- or 24-node rule is already
// converged to machine precision, and the flex marginal-slope row calculus
// evaluates O(100) such cells per row across n=10⁵–10⁶ rows per criterion
// evaluation — the fixed rule was the dominant cost of the whole fit (#979).
// `evaluate_non_affine_cell_simd` therefore walks a progressive ladder of
// rules (12, 24, 48, 96, 192, 384 nodes) and returns as soon as two
// consecutive rules agree to `NON_AFFINE_LADDER_RTOL` relative to the moment
// vector's own scale. Unlike the old fixed rule — whose error was real but
// uncertified — every accepted ladder result carries an embedded two-rule
// agreement certificate; a cell that never certifies falls through to the
// same 384-node answer the fixed rule produced.
//
// SIMD path: process 4 GL nodes per outer iteration, batching the two scalar
// `exp` calls into single 4-wide `wide::f64x4::exp` invocations. All ladder
// rule sizes are divisible by 4, so no scalar tail is needed for the GL
// sweep. The inner moment accumulation is then run scalar per-lane but with
// a 4-way unrolled slab over the moment slots to break the `z_pow *= z`
// serial dependency chain.
#[inline(always)]
fn evaluate_non_affine_cell_with_rule<const COMPUTE_VALUE: bool>(
    cell: DenestedCubicCell,
    max_degree: usize,
    gl_nodes: &[f64],
    gl_weights: &[f64],
) -> (CellMomentVec, f64) {
    let mut moments: CellMomentVec = smallvec![0.0_f64; max_degree + 1];
    let mut value_integral = 0.0_f64;
    let center = 0.5 * (cell.left + cell.right);
    let half_width = 0.5 * (cell.right - cell.left);
    let c0 = cell.c0;
    let c1 = cell.c1;
    let c2 = cell.c2;
    let c3 = cell.c3;
    let moments_slice: &mut [f64] = &mut moments;
    assert_eq!(gl_nodes.len(), gl_weights.len());
    use wide::f64x4;
    let center_v = f64x4::splat(center);
    let half_width_v = f64x4::splat(half_width);
    let c0_v = f64x4::splat(c0);
    let c1_v = f64x4::splat(c1);
    let c2_v = f64x4::splat(c2);
    let c3_v = f64x4::splat(c3);
    let neg_half_v = f64x4::splat(-0.5);
    let n_total = gl_nodes.len();
    let n_simd = n_total - (n_total % 4);
    let mut i = 0;
    while i < n_simd {
        let node_v = f64x4::from([
            gl_nodes[i],
            gl_nodes[i + 1],
            gl_nodes[i + 2],
            gl_nodes[i + 3],
        ]);
        let weight_v = f64x4::from([
            gl_weights[i],
            gl_weights[i + 1],
            gl_weights[i + 2],
            gl_weights[i + 3],
        ]);
        let z_v = half_width_v.mul_add(node_v, center_v);
        // Horner: ((c3*z + c2)*z + c1)*z + c0
        let eta_v = c3_v
            .mul_add(z_v, c2_v)
            .mul_add(z_v, c1_v)
            .mul_add(z_v, c0_v);
        let z2_v = z_v * z_v;
        let neg_q_v = neg_half_v * (z2_v + eta_v * eta_v);
        let exp_negq_v = neg_q_v.exp();
        let moment_weight_v = weight_v * exp_negq_v;
        let z_arr = z_v.to_array();
        let mw_arr = moment_weight_v.to_array();
        if COMPUTE_VALUE {
            for lane in 0..4 {
                let z = z_arr[lane];
                let mw = mw_arr[lane];
                accumulate_moments_unrolled4(moments_slice, mw, z);
                // The value integrand carries Φ(η)'s erfc, whose systematic
                // per-z error is ~1e-13. To honor the cell-value accuracy
                // contract the value term must be assembled bit-for-bit like
                // the scalar reference: a non-fused node map
                // `z_ref = center + half_width·node`, the expanded
                // `η = c0 + c1·z + c2·z² + c3·z³` (NOT the SIMD Horner-FMA used
                // for the moments), the unscaled GL weight, a scalar `exp(-½z²)`,
                // and a plain `+=`. The SIMD `z_v`/`eta_v` above (fused) feed
                // ONLY the moments and are left untouched. Any single ULP slip
                // here (FMA node map, Horner η, per-term half_width, SIMD exp,
                // FMA accumulation) drifts the 384-node sum by ~1.4e-13 and
                // breaks the contract.
                let node = gl_nodes[i + lane];
                let weight = gl_weights[i + lane];
                let z_ref = center + half_width * node;
                let eta_ref = c0 + c1 * z_ref + c2 * z_ref * z_ref + c3 * z_ref * z_ref * z_ref;
                value_integral += weight * (-0.5 * z_ref * z_ref).exp() * normal_cdf(eta_ref);
            }
        } else {
            for lane in 0..4 {
                let z = z_arr[lane];
                let mw = mw_arr[lane];
                accumulate_moments_unrolled4(moments_slice, mw, z);
            }
        }
        i += 4;
    }
    while i < n_total {
        let node = gl_nodes[i];
        let weight = gl_weights[i];
        let z = center + half_width * node;
        let eta = c3.mul_add(z, c2).mul_add(z, c1).mul_add(z, c0);
        let q = 0.5 * (z * z + eta * eta);
        let moment_weight = weight * (-q).exp();
        accumulate_moments_unrolled4(moments_slice, moment_weight, z);
        if COMPUTE_VALUE {
            // Bit-for-bit the reference value structure (see SIMD branch): the
            // node map `z = center + half_width·node` here already matches the
            // reference (non-fused), but η must use the expanded reference form
            // rather than the moment path's Horner-FMA.
            let eta_ref = c0 + c1 * z + c2 * z * z + c3 * z * z * z;
            value_integral += weight * (-0.5 * z * z).exp() * normal_cdf(eta_ref);
        }
        i += 1;
    }
    // Apply the cell half-width to both moment and value integrals ONCE at the
    // end, mirroring the prefold reference. Folding half_width per-term changes
    // f64 rounding enough to show up at the 1e-13 contract.
    for moment in moments_slice.iter_mut() {
        *moment *= half_width;
    }
    let value = if COMPUTE_VALUE {
        value_integral * half_width
    } else {
        value_integral
    };
    (moments, value)
}

/// Relative agreement threshold for the progressive non-affine quadrature
/// ladder: two consecutive Gauss-Legendre rules must agree on every moment
/// slot to this tolerance relative to the moment vector's own max magnitude
/// before the finer rule's result
/// is accepted. Gauss-Legendre error decays geometrically in the node count
/// for the analytic integrand `exp(-q(z))`, so agreement between an n-node
/// and a 2n-node rule certifies that both are converged: the coarse rule's
/// true error is bounded by the observed difference plus the (much smaller)
/// fine-rule error.
///
/// History (#979): a roundoff-floor relaxation of this test (accept when
/// successive rungs agree to `≈ n·ε·scale` rather than the bare `3e-15`) was
/// tried to let smooth cells certify below the terminal 384-node rung. It was
/// reverted: the value-bearing path carries `∫ φ(z)·Φ(η(z)) dz`, and `Φ`'s
/// `erfc` implementation has a *systematic per-z* error of order `1e-13` that
/// each rung's node set samples differently. Only the exact 384-node rule
/// reproduces the reference's erfc-noise realization, so any sub-384 rung
/// drifts from the 384 value by `≈ 1e-13` — a drift that is NOT truncation,
/// does NOT shrink with rung, and is NOT bounded by rung-to-rung agreement.
/// The moment ladder remains independent of the value integral so value- and
/// derivative-only evaluators keep returning bit-identical moments. The scalar
/// value now evaluates on the terminal 384-node rule directly, preserving the
/// `non_affine_cell_state_matches_prefold_reference_to_1e_minus_13` value
/// contract without forcing every derivative-moment caller to use the terminal
/// rung.
const NON_AFFINE_LADDER_RTOL: f64 = 1e-15;

/// Node counts of the progressive ladder below the 384-node terminal rung.
/// All divisible by 4 so the SIMD sweep needs no scalar tail.
const NON_AFFINE_LADDER_RUNGS: [usize; 5] = [12, 24, 48, 96, 192];

/// Runtime-generated Gauss-Legendre rules for the ladder rungs, computed
/// once per process by Newton iteration on the Legendre polynomial roots
/// (standard `gauleg`: cosine initial guess, 3-4 Newton steps to machine
/// precision). The terminal 384-node rung reuses the compile-time
/// `GL_NODES`/`GL_WEIGHTS` tables, which also remain the single source for
/// the GPU kernel.
fn non_affine_ladder_rules() -> &'static [(Vec<f64>, Vec<f64>)] {
    static RULES: std::sync::OnceLock<Vec<(Vec<f64>, Vec<f64>)>> = std::sync::OnceLock::new();
    RULES.get_or_init(|| {
        NON_AFFINE_LADDER_RUNGS
            .iter()
            .map(|&n| gauss_legendre_rule(n))
            .collect()
    })
}

/// Nodes and weights of the `n`-point Gauss-Legendre rule on `[-1, 1]`.
///
/// Newton iteration on `P_n` from the cosine initial guess
/// `cos(π(i + 0.75)/(n + 0.5))` converges to every root in a handful of
/// steps; weights follow from `w_i = 2 / ((1 - x_i²) P_n'(x_i)²)`. Roots are
/// filled symmetrically so the rule is exactly antisymmetric about 0.
fn gauss_legendre_rule(n: usize) -> (Vec<f64>, Vec<f64>) {
    let mut nodes = vec![0.0_f64; n];
    let mut weights = vec![0.0_f64; n];
    for i in 0..n.div_ceil(2) {
        let mut z = (std::f64::consts::PI * (i as f64 + 0.75) / (n as f64 + 0.5)).cos();
        let mut pp = 0.0_f64;
        for _ in 0..100 {
            // Legendre recurrence: p1 = P_n(z), p2 = P_{n-1}(z).
            let mut p1 = 1.0_f64;
            let mut p2 = 0.0_f64;
            for j in 1..=n {
                let p3 = p2;
                p2 = p1;
                p1 = ((2 * j - 1) as f64 * z * p2 - (j - 1) as f64 * p3) / j as f64;
            }
            pp = n as f64 * (z * p1 - p2) / (z * z - 1.0);
            let z_prev = z;
            z = z_prev - p1 / pp;
            if (z - z_prev).abs() <= f64::EPSILON {
                break;
            }
        }
        nodes[i] = -z;
        nodes[n - 1 - i] = z;
        let w = 2.0 / ((1.0 - z * z) * pp * pp);
        weights[i] = w;
        weights[n - 1 - i] = w;
    }
    (nodes, weights)
}

/// Two-rule agreement certificate for the progressive ladder. `true` when
/// every MOMENT slot agrees to `NON_AFFINE_LADDER_RTOL` relative to the fine
/// result's max magnitude. Non-finite results never certify, so they fall
/// through to the terminal 384-node rung and reproduce the fixed rule's
/// behavior exactly.
///
/// The decision is deliberately moment-only and independent of whether the
/// caller also computed the cell value: the value- and derivative-only
/// evaluators MUST select the same ladder rung so they accumulate the moment
/// vector over the same nodes and return bit-identical moments (the
/// `derivative_moment_evaluator_matches_value_evaluator_moments` invariant).
/// Value-bearing callers evaluate the scalar cell probability separately on
/// the terminal 384-node rule; this certificate governs only the reusable
/// derivative moment vector.
fn non_affine_ladder_converged(coarse: &CellMomentVec, fine: &CellMomentVec) -> bool {
    let mut scale = 0.0_f64;
    let mut err = 0.0_f64;
    for (&c, &f) in coarse.iter().zip(fine.iter()) {
        scale = scale.max(f.abs());
        err = err.max((c - f).abs());
    }
    if !(scale.is_finite() && err.is_finite()) {
        return false;
    }
    err <= NON_AFFINE_LADDER_RTOL * scale
}

/// Per-rung certification histogram for the non-affine ladder, indexed by the
/// rung that certified (`NON_AFFINE_LADDER_RUNGS[i]` at index `i`), with the
/// final slot counting cells that fell through to the terminal 384-node rule.
/// Incremented once per non-affine cell evaluation; the BMS exact-cache build
/// logs the distribution so the ladder's real cost (early-certify win vs.
/// terminal-fallthrough cost) is observable on every large-scale fit rather
/// than assumed. `+1` length for the terminal bucket.
pub(crate) static NON_AFFINE_LADDER_CERT_COUNTS: [AtomicU64; NON_AFFINE_LADDER_RUNGS.len() + 1] = [
    AtomicU64::new(0),
    AtomicU64::new(0),
    AtomicU64::new(0),
    AtomicU64::new(0),
    AtomicU64::new(0),
    AtomicU64::new(0),
];

/// Snapshot the ladder certification histogram as `(rung_node_count, count)`
/// pairs plus the terminal-fallthrough count, for logging/inspection.
pub fn non_affine_ladder_cert_histogram() -> (Vec<(usize, u64)>, u64) {
    let per_rung = NON_AFFINE_LADDER_RUNGS
        .iter()
        .enumerate()
        .map(|(i, &n)| (n, NON_AFFINE_LADDER_CERT_COUNTS[i].load(Ordering::Relaxed)))
        .collect();
    let terminal =
        NON_AFFINE_LADDER_CERT_COUNTS[NON_AFFINE_LADDER_RUNGS.len()].load(Ordering::Relaxed);
    (per_rung, terminal)
}

/// Progressive-ladder evaluation of a non-affine cell: walk the rule ladder
/// from 12 nodes upward and return the first result certified by two-rule
/// agreement; a cell that never certifies returns the terminal 384-node
/// result, byte-identical to the previous fixed-rule implementation.
#[inline]
fn evaluate_non_affine_cell_simd<const COMPUTE_VALUE: bool>(
    cell: DenestedCubicCell,
    max_degree: usize,
) -> (CellMomentVec, f64) {
    let mut prev: Option<(CellMomentVec, f64)> = None;
    for (i, (nodes, weights)) in non_affine_ladder_rules().iter().enumerate() {
        let cur =
            evaluate_non_affine_cell_with_rule::<COMPUTE_VALUE>(cell, max_degree, nodes, weights);
        if let Some(prev) = prev.as_ref()
            && non_affine_ladder_converged(&prev.0, &cur.0)
        {
            NON_AFFINE_LADDER_CERT_COUNTS[i].fetch_add(1, Ordering::Relaxed);
            return cur;
        }
        prev = Some(cur);
    }
    NON_AFFINE_LADDER_CERT_COUNTS[NON_AFFINE_LADDER_RUNGS.len()].fetch_add(1, Ordering::Relaxed);
    evaluate_non_affine_cell_with_rule::<COMPUTE_VALUE>(cell, max_degree, &GL_NODES, &GL_WEIGHTS)
}

/// Value-only evaluation of a non-affine cell on the terminal 384-node rule.
///
/// Returns the cell probability integral `∫ exp(-½z²)·Φ(η(z)) dz` (pre the
/// `1/√τ` normalization) computed bit-for-bit like the value branch of
/// [`evaluate_non_affine_cell_with_rule`]: the non-fused node map
/// `z = center + half_width·node`, the expanded (non-Horner)
/// `η = c0 + c1·z + c2·z² + c3·z³`, the unscaled GL weight, a scalar
/// `exp(-½z²)`, a plain `+=` in ascending node order, and a single trailing
/// `·half_width`. The terminal rule has 384 nodes (divisible by 4), so the
/// general kernel's value path never takes its scalar tail — this loop walks
/// the same nodes in the same order and therefore reproduces the reference
/// erfc-noise realization the `1e-13` value contract pins down.
///
/// Computing this through `evaluate_non_affine_cell_with_rule::<true>` at
/// `max_degree = 0` would additionally run the 4-wide SIMD `exp(-q)` moment
/// sweep and a moment accumulation on every node only to discard the moment
/// vector. The survival marginal-slope fit evaluates a value per non-affine
/// partition cell, so that discarded moment work is the dominant waste in the
/// per-cell pass; this evaluator does only the work the value needs.
fn evaluate_non_affine_cell_value_terminal(cell: DenestedCubicCell) -> f64 {
    let center = 0.5 * (cell.left + cell.right);
    let half_width = 0.5 * (cell.right - cell.left);
    let c0 = cell.c0;
    let c1 = cell.c1;
    let c2 = cell.c2;
    let c3 = cell.c3;
    let mut value_integral = 0.0_f64;
    for (&node, &weight) in GL_NODES.iter().zip(GL_WEIGHTS.iter()) {
        let z = center + half_width * node;
        let eta = c0 + c1 * z + c2 * z * z + c3 * z * z * z;
        value_integral += weight * (-0.5 * z * z).exp() * normal_cdf(eta);
    }
    value_integral * half_width
}

fn evaluate_non_affine_cell_state(
    cell: DenestedCubicCell,
    branch: ExactCellBranch,
    max_degree: usize,
) -> Result<CellMomentState, String> {
    let (moments, _) = evaluate_non_affine_cell_simd::<false>(cell, max_degree);
    let value_integral = evaluate_non_affine_cell_value_terminal(cell);
    // Reference structure: `value_integral * half_width / sqrt(TAU)`. The
    // half_width factor is already applied inside the rule evaluator, so divide
    // by sqrt(TAU) here (a true division, NOT multiply-by-reciprocal) to
    // reproduce the reference's final rounding bit-for-bit.
    Ok(CellMomentState {
        branch,
        value: value_integral / (std::f64::consts::TAU).sqrt(),
        moments,
    })
}

fn evaluate_non_affine_cell_derivative_state(
    cell: DenestedCubicCell,
    branch: ExactCellBranch,
    max_degree: usize,
) -> Result<CellDerivativeMomentState, String> {
    let (moments, _) = evaluate_non_affine_cell_simd::<false>(cell, max_degree);
    Ok(CellDerivativeMomentState { branch, moments })
}

/// De-nested cubic cell evaluator.
///
/// Affine cells use the closed-form affine anchor; non-affine cells (Quartic
/// and Sextic branches) are evaluated in a single pass over a fixed
/// high-order Gauss-Legendre rule on `[left, right]`.
pub fn evaluate_cell_moments(
    cell: DenestedCubicCell,
    max_degree: usize,
) -> Result<CellMomentState, String> {
    if !TAIL_CELL_MOMENT_CACHE_ENABLED.load(std::sync::atomic::Ordering::Relaxed) {
        return evaluate_cell_moments_uncached(cell, max_degree);
    }
    tail_cell_moment_cache().evaluate(cell, max_degree)
}

/// Evaluate cell moments without consulting the global affine-tail memo.
///
/// This is retained for regression tests and before/after microbenchmarks;
/// production callers should use [`evaluate_cell_moments`].
pub fn evaluate_cell_moments_uncached(
    cell: DenestedCubicCell,
    max_degree: usize,
) -> Result<CellMomentState, String> {
    evaluate_cell_state_dispatched(
        cell,
        max_degree,
        evaluate_affine_cell_state,
        evaluate_non_affine_cell_state,
    )
}

/// Evaluate only the moment vector needed by derivative contractions.
///
/// This deliberately does not compute the cell probability value
/// `∫ φ(z) Φ(η(z)) dz`. Derivative contractions consume
/// `∫ z^k exp(-q(z)) dz` moments only, so keeping the value out of the return
/// type prevents this cheaper evaluator from satisfying value-bearing calls.
pub fn evaluate_cell_derivative_moments_uncached(
    cell: DenestedCubicCell,
    max_degree: usize,
) -> Result<CellDerivativeMomentState, String> {
    evaluate_cell_state_dispatched(
        cell,
        max_degree,
        evaluate_affine_cell_derivative_state,
        evaluate_non_affine_cell_derivative_state,
    )
}

/// Shared branch dispatch for the value-bearing and derivative-only cell
/// evaluators. Both walk the same decision tree (semi-infinite tail → must
/// be affine; finite cell → branch-by-coefficients with the sextic
/// degenerate-lowering path), differing only in which pair of
/// `(affine, non_affine)` evaluator helpers to delegate to.  The two helpers
/// are passed as `fn` pointers so the dispatch monomorphizes per `S` and
/// keeps the existing pre-condition errors / unreachable branch handling
/// in lockstep across both evaluators.
fn evaluate_cell_state_dispatched<S>(
    cell: DenestedCubicCell,
    max_degree: usize,
    affine: fn(DenestedCubicCell, usize) -> Result<S, String>,
    non_affine: fn(DenestedCubicCell, ExactCellBranch, usize) -> Result<S, String>,
) -> Result<S, String> {
    let left_inf = !cell.left.is_finite();
    let right_inf = !cell.right.is_finite();
    if left_inf || right_inf {
        // Semi-infinite tail cells must be affine: the deviation saturates
        // to a constant outside support, so c2=c3=0.  Both the BVN CDF
        // and the truncated-Gaussian moment vector handle infinite bounds.
        if cell.c2.abs() > NORMALIZED_CELL_BRANCH_TOL || cell.c3.abs() > NORMALIZED_CELL_BRANCH_TOL
        {
            return Err(CubicCellKernelError::invalid_cell_shape(format!(
                "semi-infinite cell [{}, {}] must be affine (c2=c3=0), got c2={:.3e}, c3={:.3e}",
                cell.left, cell.right, cell.c2, cell.c3
            ))
            .into());
        }
        return affine(cell, max_degree);
    }
    if cell.right <= cell.left {
        return Err(CubicCellKernelError::invalid_cell_shape(format!(
            "finite cell must have left < right, got [{}, {}]",
            cell.left, cell.right
        ))
        .into());
    }
    let branch = branch_cell(cell)?;
    if branch == ExactCellBranch::Affine {
        return affine(cell, max_degree);
    }
    if branch == ExactCellBranch::Sextic {
        let lead = sextic_qprime_coefficients(cell.c0, cell.c1, cell.c2, cell.c3)[5];
        if !lead.is_finite() {
            return Err(CubicCellKernelError::invalid_cell_shape(format!(
                "sextic cell evaluation encountered non-finite leading coefficient: {lead:.3e}"
            ))
            .into());
        }
        if let Some(lower_branch) = degenerate_sextic_branch(cell, lead)? {
            return match lower_branch {
                ExactCellBranch::Quartic => non_affine(
                    DenestedCubicCell { c3: 0.0, ..cell },
                    ExactCellBranch::Quartic,
                    max_degree,
                ),
                ExactCellBranch::Affine => affine(
                    DenestedCubicCell {
                        c2: 0.0,
                        c3: 0.0,
                        ..cell
                    },
                    max_degree,
                ),
                ExactCellBranch::Sextic => Err(CubicCellKernelError::invalid_cell_shape(
                    "internal: degenerate_sextic_branch returned Sextic as a lowered branch",
                )
                .into()),
            };
        }
    }
    non_affine(cell, branch, max_degree)
}

/// Evaluate a de-nested cubic cell through a fit-lifetime byte-limited LRU cache.
///
/// The fingerprint is an exact bit-cast of `(c0, c1, c2, c3, left, right)`, so
/// eviction and reuse cannot alias nearby-but-different cells.  A cached entry
/// computed to a higher degree may satisfy a lower-degree request by truncating
/// the moment vector, preserving the public [`evaluate_cell_moments`] contract.
pub fn evaluate_cell_moments_cached(
    cell: DenestedCubicCell,
    max_degree: usize,
    cache: &CellMomentLruCache,
    stats: Option<&CellMomentCacheStats>,
) -> Result<CellMomentState, String> {
    // Affine cells (every rigid-path cell and every tail cell) evaluate
    // through the closed-form anchor — cheaper than a single LRU probe. The
    // LRU exists only to amortize the EXPENSIVE non-affine transport across
    // recurring cells; at large n the row scalars `(a, b)` are unique per
    // row, so affine cells never recur and routing them through the sharded
    // mutex was pure cost (320k lock+insert+evict ops per gradient eval, ~0%
    // hit — the dominant cost of the rigid n=320k fit, #979). Bypass the
    // cache entirely for them.
    if matches!(branch_cell(cell), Ok(ExactCellBranch::Affine)) {
        if let Some(stats) = stats {
            stats.misses.fetch_add(1, Ordering::Relaxed);
        }
        return evaluate_cell_moments_uncached(cell, max_degree);
    }
    let key = CellFingerprint::new(cell);
    let existing_derivative = match cache.get(&key) {
        Some(cached) => {
            if let Some(state) = cached.state_for_degree(max_degree) {
                if let Some(stats) = stats {
                    stats.hits.fetch_add(1, Ordering::Relaxed);
                }
                return Ok(state);
            }
            // `cached.derivative_state` is `Option<Arc<_>>`; `.clone()` here
            // is the cheap refcount bump the audit-39 fix targets, not a
            // full moment-vector deep clone.
            cached.derivative_state.clone()
        }
        None => None,
    };
    if let Some(stats) = stats {
        stats.misses.fetch_add(1, Ordering::Relaxed);
    }
    let state = evaluate_cell_moments(cell, max_degree)?;
    // Wrap the freshly-computed state in `Arc` once, share it with the cache
    // through `Arc::clone`, and return the underlying value by unwrapping the
    // unique-reference (caller-side) `Arc`. This replaces the prior
    // `state.clone()` deep copy at the insert site.
    let shared = Arc::new(state);
    let mut entry = CachedCellMoments::new(Arc::clone(&shared));
    if let Some(derivative) = existing_derivative {
        entry = entry.with_derivative(derivative);
    }
    cache.insert(key, entry);
    Ok(Arc::try_unwrap(shared).unwrap_or_else(|a| (*a).clone()))
}

/// Derivative-moment counterpart to [`evaluate_cell_moments_cached`]. Shares
/// the value-moment LRU by storing both moment kinds in a single
/// [`CachedCellMoments`] entry keyed on the cell fingerprint — derivative
/// insertions preserve any pre-existing value state and vice versa, so the
/// two callers never evict each other's work.
pub fn evaluate_cell_derivative_moments_cached(
    cell: DenestedCubicCell,
    max_degree: usize,
    cache: &CellMomentLruCache,
    stats: Option<&CellMomentCacheStats>,
) -> Result<CellDerivativeMomentState, String> {
    // Affine cells bypass the LRU — see `evaluate_cell_moments_cached` for
    // why the sharded-mutex memo is pure overhead on the closed-form affine
    // path at large n (#979).
    if matches!(branch_cell(cell), Ok(ExactCellBranch::Affine)) {
        if let Some(stats) = stats {
            stats.misses.fetch_add(1, Ordering::Relaxed);
        }
        return evaluate_cell_derivative_moments_uncached(cell, max_degree);
    }
    let key = CellFingerprint::new(cell);
    let existing_value = match cache.get(&key) {
        Some(cached) => {
            if let Some(state) = cached.derivative_state_for_degree(max_degree) {
                if let Some(stats) = stats {
                    stats.hits.fetch_add(1, Ordering::Relaxed);
                }
                return Ok(state);
            }
            // `cached.state` is `Option<Arc<_>>`; `.clone()` here is the cheap
            // refcount bump the audit-39 fix targets, not a full moment-vector
            // deep clone.
            cached.state.clone()
        }
        None => None,
    };
    if let Some(stats) = stats {
        stats.misses.fetch_add(1, Ordering::Relaxed);
    }
    let state = evaluate_cell_derivative_moments_uncached(cell, max_degree)?;
    // Wrap the freshly-computed state in `Arc` once, share it with the cache
    // through `Arc::clone`, and return the underlying value by unwrapping the
    // unique-reference (caller-side) `Arc`. This replaces the prior
    // `state.clone()` deep copy at the insert site.
    let shared = Arc::new(state);
    let mut entry = CachedCellMoments::new_derivative(Arc::clone(&shared));
    if let Some(value) = existing_value {
        entry = entry.with_value(value);
    }
    cache.insert(key, entry);
    Ok(Arc::try_unwrap(shared).unwrap_or_else(|a| (*a).clone()))
}

/// Scratch-backed variant of [`evaluate_cell_moments`].
///
/// Reuses the supplied [`CellMomentScratch`] for the returned moments slice,
/// so repeated calls with the same scratch (and a sufficient initial capacity)
/// avoid per-call `Vec` allocations on the hot inner-PIRLS row-intercept
/// solver path. Internal transport allocations are unchanged.
pub fn evaluate_cell_moments_with_scratch<'a>(
    cell: DenestedCubicCell,
    max_degree: usize,
    scratch: &'a mut CellMomentScratch,
) -> Result<CellMomentStateRef<'a>, String> {
    let state = evaluate_cell_moments(cell, max_degree)?;
    let out = scratch.prepare_moments(max_degree + 1);
    out.copy_from_slice(&state.moments);
    Ok(CellMomentStateRef {
        branch: state.branch,
        value: state.value,
        moments: out,
    })
}

#[cfg(test)]
mod tests {
    use super::*;
    use gam_math::probability::normal_pdf;

    #[inline]
    pub(super) fn polynomial_value(coefficients: &[f64], z: f64) -> f64 {
        coefficients
            .iter()
            .rev()
            .fold(0.0, |acc, &coeff| acc * z + coeff)
    }

    fn reset_cell_moment_test_reallocs() {
        super::CELL_MOMENT_REALLOCS.store(0, std::sync::atomic::Ordering::Relaxed);
    }

    fn cell_moment_test_reallocs() -> usize {
        super::CELL_MOMENT_REALLOCS.load(std::sync::atomic::Ordering::Relaxed)
    }

    fn assert_close_rel(label: &str, actual: f64, expected: f64, tol: f64) {
        let denom = expected.abs().max(1.0);
        let rel = (actual - expected).abs() / denom;
        assert!(
            rel <= tol,
            "{label}: actual={actual:.17e} expected={expected:.17e} rel={rel:.3e} tol={tol:.3e}"
        );
    }

    // The link-basis cell coefficient `transformed_link_cubic(span, a, b)` is, in
    // each of its four output components, a polynomial of TOTAL degree exactly 3 in
    // (a, b):
    //   d0 = c0 + c1·s + c2·s² + c3·s³            (s = a − left; deg 3 in a)
    //   d1 = b·(c1 + 2c2·s + 3c3·s²)              (a²·b → total deg 3)
    //   d2 = b²·(c2 + 3c3·s)                       (a·b² → total deg 3)
    //   d3 = c3·b³                                 (b³  → total deg 3)
    // Therefore EVERY 4th-order total (a,b)-partial (∂⁴/∂aⁱ∂b^{4−i}) is identically
    // zero, while the 3rd-order partials (∂³/∂aⁱ∂b^{3−i}) are the highest nonzero
    // ones. This is the exact algebraic fact the bidirectional flex jet relies on:
    // a "second mixed derivative of a third-a-partial" slot, etc., demands a 4th
    // total (a,b)-partial and must be hard-zero — substituting a (nonzero) 3rd
    // partial there is a bug. This test certifies BOTH facts by central FD so the
    // hard-coded `0.0` fixes are provably correct and provably necessary.
    #[test]
    fn link_basis_cell_fourth_ab_partials_vanish_third_are_nonzero() {
        let span = LocalSpanCubic {
            left: -0.4,
            right: 1.6,
            c0: 0.37,
            c1: -0.81,
            c2: 0.53,
            c3: -0.29,
        };
        let a0 = 0.23_f64;
        let b0 = 0.61_f64;
        let h = 1e-2_f64;

        // Generic central-difference stencils per derivative order.
        let stencil = |order: usize| -> &'static [(i64, f64)] {
            match order {
                0 => &[(0, 1.0)],
                1 => &[(-1, -0.5), (1, 0.5)],
                2 => &[(-1, 1.0), (0, -2.0), (1, 1.0)],
                3 => &[(-2, -0.5), (-1, 1.0), (1, -1.0), (2, 0.5)],
                4 => &[(-2, 1.0), (-1, -4.0), (0, 6.0), (1, -4.0), (2, 1.0)],
                _ => &[(0, 1.0)],
            }
        };
        // FD of component `k` of the cell coefficient: ∂^{na+nb}/∂a^{na}∂b^{nb}.
        let fd = |k: usize, na: usize, nb: usize| -> f64 {
            let mut acc = 0.0;
            for &(ia, wa) in stencil(na) {
                for &(ib, wb) in stencil(nb) {
                    let a = a0 + (ia as f64) * h;
                    let b = b0 + (ib as f64) * h;
                    acc += wa * wb * link_basis_cell_coefficients(span, a, b)[k];
                }
            }
            acc / h.powi((na + nb) as i32)
        };

        let (p3_aaa, p3_aab, p3_abb, p3_bbb) = link_basis_cell_third_partials(span);

        // (1) The analytic 3rd partials match FD (within FD truncation) — and at
        // least one is appreciably nonzero, so these are real signal that a wrong
        // slot would inject.
        let mut max_third = 0.0_f64;
        for k in 0..4 {
            for (label, (na, nb), analytic) in [
                ("aaa", (3usize, 0usize), p3_aaa[k]),
                ("aab", (2, 1), p3_aab[k]),
                ("abb", (1, 2), p3_abb[k]),
                ("bbb", (0, 3), p3_bbb[k]),
            ] {
                let got = fd(k, na, nb);
                assert!(
                    (got - analytic).abs() <= 1e-4 + 1e-3 * analytic.abs(),
                    "3rd partial {label}[{k}] analytic {analytic:+.6e} vs FD {got:+.6e}"
                );
                max_third = max_third.max(analytic.abs());
            }
        }
        assert!(
            max_third > 1e-1,
            "expected an appreciable nonzero 3rd (a,b)-partial; max |analytic| = {max_third:.3e}"
        );

        // (2) EVERY 4th-order total (a,b)-partial vanishes (degree-3 polynomial),
        // certifying that the hard-coded `0.0` in the bidirectional d12 slots is the
        // mathematically required value, not an approximation.
        for k in 0..4 {
            for (na, nb) in [(4usize, 0usize), (3, 1), (2, 2), (1, 3), (0, 4)] {
                let got = fd(k, na, nb);
                assert!(
                    got.abs() <= 1e-2,
                    "4th (a,b)-partial ∂^{na}_a∂^{nb}_b of cell coeff[{k}] must vanish, FD = {got:+.6e}"
                );
            }
        }
    }

    #[test]
    fn non_affine_cell_state_grid_matches_public_cell_moments_reference() {
        let cells = [
            DenestedCubicCell {
                left: -1.25,
                right: -0.2,
                c0: -0.35,
                c1: 0.85,
                c2: 0.04,
                c3: -0.015,
            },
            DenestedCubicCell {
                left: -0.2,
                right: 0.55,
                c0: 0.12,
                c1: -0.65,
                c2: -0.025,
                c3: 0.02,
            },
            DenestedCubicCell {
                left: 0.55,
                right: 1.6,
                c0: 0.42,
                c1: 0.35,
                c2: 0.018,
                c3: 0.012,
            },
        ];
        for cell in cells {
            let branch = branch_cell(cell).expect("branch");
            assert_ne!(branch, ExactCellBranch::Affine);
            for max_degree in [0usize, 2, 4, 9, 16] {
                let direct = evaluate_non_affine_cell_state(cell, branch, max_degree)
                    .expect("direct non-affine transport");
                let public = evaluate_cell_moments(cell, max_degree).expect("public evaluator");
                assert_eq!(direct.branch, public.branch);
                assert_eq!(direct.moments.len(), public.moments.len());
                let value_scale = direct.value.abs().max(public.value.abs()).max(1.0);
                assert!(
                    (direct.value - public.value).abs() <= 1e-10 * value_scale,
                    "value mismatch for {cell:?} degree {max_degree}: direct={} public={}",
                    direct.value,
                    public.value
                );
                for (degree, (lhs, rhs)) in
                    direct.moments.iter().zip(public.moments.iter()).enumerate()
                {
                    let scale = lhs.abs().max(rhs.abs()).max(1.0);
                    assert!(
                        (lhs - rhs).abs() <= 1e-10 * scale,
                        "moment {degree} mismatch for {cell:?} degree {max_degree}: {lhs} vs {rhs}"
                    );
                }
            }
        }
    }

    #[test]
    fn affine_tail_cell_memo_matches_uncached_grid_and_records_hits() {
        // Use a dedicated local cache so the test's hit/miss/entry counters
        // are not perturbed by concurrent tests that drive the shared
        // global memo through `evaluate_cell_moments`. Asserting on the
        // global counters made this test race-flaky when the suite ran in
        // parallel.
        let cache = TailCellMomentCache::new();
        let c0s = [-2.0, -0.25, 0.0, 1.5];
        let c1s = [-1.2, -0.05, 0.0, 0.8];
        let endpoints = [-4.0, -1.0, 0.0, 2.5, 6.0];
        let degrees = [0_usize, 4, 9, 16, 24];

        for &c0 in &c0s {
            for &c1 in &c1s {
                for &endpoint in &endpoints {
                    for &max_degree in &degrees {
                        for &(left, right) in
                            &[(f64::NEG_INFINITY, endpoint), (endpoint, f64::INFINITY)]
                        {
                            let cell = DenestedCubicCell {
                                left,
                                right,
                                c0,
                                c1,
                                c2: 0.0,
                                c3: 0.0,
                            };
                            let expected = evaluate_cell_moments_uncached(cell, max_degree)
                                .expect("uncached affine tail moments");
                            let actual = cache
                                .evaluate(cell, max_degree)
                                .expect("cached affine tail moments miss");
                            let repeat = cache
                                .evaluate(cell, max_degree)
                                .expect("cached affine tail moments hit");
                            assert_eq!(actual.branch, expected.branch);
                            assert_eq!(repeat.branch, expected.branch);
                            assert_close_rel(
                                "tail value miss",
                                actual.value,
                                expected.value,
                                1e-14,
                            );
                            assert_close_rel("tail value hit", repeat.value, expected.value, 1e-14);
                            assert_eq!(actual.moments.len(), expected.moments.len());
                            assert_eq!(repeat.moments.len(), expected.moments.len());
                            for (idx, ((a, r), e)) in actual
                                .moments
                                .iter()
                                .zip(repeat.moments.iter())
                                .zip(expected.moments.iter())
                                .enumerate()
                            {
                                assert_close_rel(
                                    &format!("tail moment miss[{idx}]"),
                                    *a,
                                    *e,
                                    1e-14,
                                );
                                assert_close_rel(&format!("tail moment hit[{idx}]"), *r, *e, 1e-14);
                            }
                        }
                    }
                }
            }
        }

        let stats = cache.stats();
        assert_eq!(stats.misses, stats.entries);
        assert!(
            stats.hits >= stats.misses,
            "expected repeat hits: {stats:?}"
        );
        assert!(
            stats.hit_rate() >= 0.5,
            "unexpected low hit rate: {stats:?}"
        );
    }

    fn reference_bivariate_normal_cdf_20(h: f64, k: f64, rho: f64) -> f64 {
        if h == f64::NEG_INFINITY || k == f64::NEG_INFINITY {
            return 0.0;
        }
        if h == f64::INFINITY {
            return normal_cdf(k);
        }
        if k == f64::INFINITY {
            return normal_cdf(h);
        }
        let rho_clamped = rho.clamp(-1.0, 1.0);
        if rho_clamped >= 1.0 - 1e-12 {
            return normal_cdf(h.min(k));
        }
        if rho_clamped <= -1.0 + 1e-12 {
            return (normal_cdf(h) - normal_cdf(-k)).clamp(0.0, 1.0);
        }

        let hs = 0.5 * (h * h + k * k);
        let asr = rho_clamped.asin();
        let mut sum = 0.0;
        for (&node, &weight) in GL20_NODES.iter().zip(GL20_WEIGHTS.iter()) {
            let sn = (0.5 * asr * (node + 1.0)).sin();
            let one_minus = 1.0 - sn * sn;
            let expo = ((sn * h * k) - hs) / one_minus;
            sum += weight * expo.exp();
        }
        (normal_cdf(h) * normal_cdf(k) + asr * sum / (4.0 * std::f64::consts::PI)).clamp(0.0, 1.0)
    }

    #[test]
    fn non_affine_cell_state_reference_grid_matches_public_moments() {
        let c0s = [-0.4, 0.0, 0.35];
        let c1s = [-0.8, 0.25, 1.1];
        let c2s = [-0.12, 0.08];
        let c3s = [-0.04, 0.03];
        let intervals = [(-1.25, -0.2), (-0.5, 0.75), (0.1, 1.4)];
        let degrees = [3usize, 6, 9, 12];

        for &c0 in &c0s {
            for &c1 in &c1s {
                for &c2 in &c2s {
                    for &c3 in &c3s {
                        for &(left, right) in &intervals {
                            let cell = DenestedCubicCell {
                                left,
                                right,
                                c0,
                                c1,
                                c2,
                                c3,
                            };
                            let branch = branch_cell(cell).expect("branch");
                            assert_ne!(branch, ExactCellBranch::Affine);
                            for &degree in &degrees {
                                let direct = evaluate_non_affine_cell_state(cell, branch, degree)
                                    .expect("direct non-affine state");
                                let public = evaluate_cell_moments(cell, degree)
                                    .expect("public non-affine state");
                                assert_eq!(direct.branch, public.branch);
                                let value_scale =
                                    direct.value.abs().max(public.value.abs()).max(1.0);
                                assert!(
                                    (direct.value - public.value).abs() / value_scale <= 1.0e-15,
                                    "value mismatch for {cell:?}, degree {degree}: direct={:.17e}, public={:.17e}",
                                    direct.value,
                                    public.value
                                );
                                assert_eq!(direct.moments.len(), public.moments.len());
                                for (idx, (&a, &b)) in
                                    direct.moments.iter().zip(public.moments.iter()).enumerate()
                                {
                                    let scale = a.abs().max(b.abs()).max(1.0);
                                    assert!(
                                        (a - b).abs() / scale <= 1.0e-15,
                                        "moment {idx} mismatch for {cell:?}, degree {degree}: direct={a:.17e}, public={b:.17e}"
                                    );
                                }
                            }
                        }
                    }
                }
            }
        }
    }

    #[test]
    fn bivariate_normal_cdf_matches_reference_grid_to_1e_minus_10() {
        let hs = [-8.0, -5.0, -3.0, -1.5, -0.5, 0.0, 0.25, 1.0, 2.5, 5.0, 8.0];
        let ks = [-8.0, -4.0, -2.0, -0.75, 0.0, 0.4, 1.25, 3.0, 6.0, 8.0];
        let rhos = [
            -0.999_999_999_999,
            -0.999,
            -0.95,
            -0.7,
            -0.3,
            -1.0e-12,
            0.0,
            1.0e-12,
            0.3,
            0.7,
            0.95,
            0.999,
            0.999_999_999_999,
        ];
        for &h in &hs {
            for &k in &ks {
                for &rho in &rhos {
                    let actual = bivariate_normal_cdf(h, k, rho).expect("bvn");
                    let expected = reference_bivariate_normal_cdf_20(h, k, rho);
                    let scale = expected.abs().max(1.0e-300);
                    let rel = (actual - expected).abs() / scale;
                    assert!(
                        rel < 1.0e-10 || (actual - expected).abs() < 1.0e-14,
                        "h={h} k={k} rho={rho} actual={actual:.17e} expected={expected:.17e} rel={rel:.3e}"
                    );
                }
            }
        }
    }

    #[test]
    fn bivariate_normal_cdf_matches_reference_lcg_property_samples() {
        let mut seed = 0x5eed_cafe_f00d_u64;
        let mut next_unit = || {
            seed = seed.wrapping_mul(6_364_136_223_846_793_005).wrapping_add(1);
            ((seed >> 11) as f64) * (1.0 / ((1_u64 << 53) as f64))
        };
        for _ in 0..4096 {
            let h = -8.0 + 16.0 * next_unit();
            let k = -8.0 + 16.0 * next_unit();
            let rho = -0.999 + 1.998 * next_unit();
            let actual = bivariate_normal_cdf(h, k, rho).expect("bvn");
            let expected = reference_bivariate_normal_cdf_20(h, k, rho);
            let scale = expected.abs().max(1.0e-300);
            let rel = (actual - expected).abs() / scale;
            assert!(
                rel < 1.0e-10 || (actual - expected).abs() < 1.0e-14,
                "h={h} k={k} rho={rho} actual={actual:.17e} expected={expected:.17e} rel={rel:.3e}"
            );
        }
    }

    #[test]
    fn affine_bvn_interval_primitive_matches_two_cdf_difference() {
        let hs = [-6.0, -2.0, -0.25, 0.0, 0.8, 3.0, 6.0];
        let bounds = [
            (-5.0, -2.0),
            (-3.0, -0.1),
            (-1.0, 0.0),
            (-0.25, 0.75),
            (0.2, 3.5),
            (2.0, 7.0),
        ];
        let rhos = [-0.98, -0.8, -0.25, 0.0, 0.25, 0.8, 0.98];
        for &h in &hs {
            for &(left, right) in &bounds {
                for &rho in &rhos {
                    let actual =
                        bivariate_normal_cdf_interval(h, left, right, rho).expect("interval");
                    let expected = (reference_bivariate_normal_cdf_20(h, right, rho)
                        - reference_bivariate_normal_cdf_20(h, left, rho))
                    .clamp(0.0, 1.0);
                    let scale = expected.abs().max(1.0e-300);
                    let rel = (actual - expected).abs() / scale;
                    assert!(
                        rel < 1.0e-10 || (actual - expected).abs() < 1.0e-12,
                        "h={h} left={left} right={right} rho={rho} actual={actual:.17e} expected={expected:.17e} rel={rel:.3e}"
                    );
                }
            }
        }
    }

    fn simpson_integral<F>(left: f64, right: f64, steps: usize, f: F) -> f64
    where
        F: Fn(f64) -> f64,
    {
        let n = if steps.is_multiple_of(2) {
            steps
        } else {
            steps + 1
        };
        let h = (right - left) / n as f64;
        let mut acc = f(left) + f(right);
        for k in 1..n {
            let x = left + h * k as f64;
            let w = if k % 2 == 0 { 2.0 } else { 4.0 };
            acc += w * f(x);
        }
        acc * h / 3.0
    }

    #[test]
    fn global_transform_preserves_local_span_polynomial() {
        let span = LocalSpanCubic {
            left: -1.2,
            right: 0.8,
            c0: 0.3,
            c1: -0.25,
            c2: 0.11,
            c3: -0.04,
        };
        let (g0, g1, g2, g3) = global_cubic_from_local(span);
        for &x in &[-1.2, -0.7, -0.1, 0.4, 0.8] {
            let local = span.evaluate(x);
            let global = g0 + g1 * x + g2 * x * x + g3 * x * x * x;
            assert!((local - global).abs() < 1e-12);
        }
    }

    #[test]
    fn bivariate_normal_cdf_independent_factorizes() {
        let h = -0.35;
        let k = 0.8;
        let out = bivariate_normal_cdf(h, k, 0.0).expect("bvn");
        let target = normal_cdf(h) * normal_cdf(k);
        assert!((out - target).abs() < 1e-12);
    }

    #[test]
    fn evaluate_affine_cell_state_matches_numeric_integrals() {
        let cell = DenestedCubicCell {
            left: -0.9,
            right: 0.8,
            c0: 0.15,
            c1: -0.35,
            c2: 0.0,
            c3: 0.0,
        };
        let state = evaluate_affine_cell_state(cell, 6).expect("affine cell");
        let value_numeric = simpson_integral(cell.left, cell.right, 4000, |z| {
            super::normal_cdf(cell.eta(z)) * normal_pdf(z)
        });
        assert_eq!(state.branch, ExactCellBranch::Affine);
        assert!((state.value - value_numeric).abs() < 1e-9);
        for degree in 0..=6 {
            let target = simpson_integral(cell.left, cell.right, 4000, |z| {
                z.powi(degree as i32) * (-cell.q(z)).exp()
            });
            assert!((state.moments[degree] - target).abs() < 1e-9);
        }
    }

    #[test]
    fn affine_cell_value_matches_zero_moment_derivative() {
        let cell = DenestedCubicCell {
            left: -1.1,
            right: 0.7,
            c0: 0.23,
            c1: -0.41,
            c2: 0.0,
            c3: 0.0,
        };
        let h = 1e-6;
        let plus = evaluate_affine_cell_state(
            DenestedCubicCell {
                c0: cell.c0 + h,
                ..cell
            },
            0,
        )
        .expect("affine plus");
        let minus = evaluate_affine_cell_state(
            DenestedCubicCell {
                c0: cell.c0 - h,
                ..cell
            },
            0,
        )
        .expect("affine minus");
        let center = evaluate_affine_cell_state(cell, 0).expect("affine center");
        let d_value = (plus.value - minus.value) / (2.0 * h);
        let target = INV_TWO_PI * center.moments[0];
        assert!((d_value - target).abs() < 1e-8);
    }

    #[test]
    fn coefficient_partials_match_exact_span_derivatives() {
        let score_span = LocalSpanCubic {
            left: -0.75,
            right: 0.25,
            c0: 0.08,
            c1: -0.03,
            c2: 0.02,
            c3: -0.01,
        };
        let link_span = LocalSpanCubic {
            left: -0.6,
            right: 0.9,
            c0: -0.05,
            c1: 0.04,
            c2: -0.02,
            c3: 0.015,
        };
        let a = 0.3;
        let b = -0.7;
        let (dc_da, dc_db) = denested_cell_coefficient_partials(score_span, link_span, a, b);
        for &z in &[-0.75, -0.4, -0.1, 0.2] {
            let u = a + b * z;
            let eta_a = 1.0 + link_span.first_derivative(u);
            let eta_b = z + score_span.evaluate(z) + z * link_span.first_derivative(u);
            assert!((polynomial_value(&dc_da, z) - eta_a).abs() < 1e-12);
            assert!((polynomial_value(&dc_db, z) - eta_b).abs() < 1e-12);
        }
    }

    #[test]
    fn second_coefficient_partials_match_exact_span_derivatives() {
        let score_span = LocalSpanCubic {
            left: -0.75,
            right: 0.25,
            c0: 0.08,
            c1: -0.03,
            c2: 0.02,
            c3: -0.01,
        };
        let link_span = LocalSpanCubic {
            left: -0.6,
            right: 0.9,
            c0: -0.05,
            c1: 0.04,
            c2: -0.02,
            c3: 0.015,
        };
        let a = 0.3;
        let b = -0.7;
        let second_partials = denested_cell_second_partials(score_span, link_span, a, b);
        let dc_daa = second_partials.0;
        let dc_dab = second_partials.1;
        let dc_dbb = second_partials.2;
        for &z in &[-0.75, -0.4, -0.1, 0.2] {
            let u = a + b * z;
            let eta_aa = link_span.second_derivative(u);
            let eta_ab = z * link_span.second_derivative(u);
            let eta_bb = z * z * link_span.second_derivative(u);
            assert!((polynomial_value(&dc_daa, z) - eta_aa).abs() < 1e-12);
            assert!((polynomial_value(&dc_dab, z) - eta_ab).abs() < 1e-12);
            assert!((polynomial_value(&dc_dbb, z) - eta_bb).abs() < 1e-12);
        }
    }

    #[test]
    fn higher_derivative_moment_helpers_reject_empty_first_coefficients() {
        let cell = DenestedCubicCell {
            left: -1.0,
            right: 1.0,
            c0: 0.0,
            c1: 1.0,
            c2: 0.0,
            c3: 0.0,
        };
        let moments = [1.0; 16];

        let third_err = cell_third_derivative_from_moments(
            cell,
            &[],
            &[1.0],
            &[1.0],
            &[],
            &[],
            &[],
            &[],
            &moments,
        )
        .expect_err("empty first coefficients should be rejected");
        assert!(third_err.contains("r first-derivative coefficients must be non-empty"));

        let fourth_err = cell_fourth_derivative_from_moments(
            cell,
            &[1.0],
            &[],
            &[1.0],
            &[1.0],
            &[],
            &[],
            &[],
            &[],
            &[],
            &[],
            &[],
            &[],
            &[],
            &[],
            &[],
            &moments,
        )
        .expect_err("empty first coefficients should be rejected");
        assert!(fourth_err.contains("s first-derivative coefficients must be non-empty"));
    }

    #[test]
    fn fourth_derivative_rejects_overlong_scratch_convolutions() {
        let cell = DenestedCubicCell {
            left: -1.0,
            right: 1.0,
            c0: 0.0,
            c1: 1.0,
            c2: 0.0,
            c3: 0.0,
        };
        let long_first = [1.0; 10];
        let zero = [0.0; 1];
        let moments = [1.0; 64];

        let err = cell_fourth_derivative_from_moments(
            cell,
            &long_first,
            &long_first,
            &long_first,
            &long_first,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &moments,
        )
        .expect_err("oversized convolution should be rejected before writing scratch");
        assert!(err.contains("fourth derivative polynomial convolution scratch too small"));
    }

    #[test]
    fn score_and_link_basis_cell_coefficients_match_direct_construction() {
        let score_basis_span = LocalSpanCubic {
            left: -0.7,
            right: 0.4,
            c0: 0.2,
            c1: -0.04,
            c2: 0.03,
            c3: -0.01,
        };
        let link_basis_span = LocalSpanCubic {
            left: -0.5,
            right: 1.1,
            c0: -0.03,
            c1: 0.05,
            c2: -0.02,
            c3: 0.01,
        };
        let a = 0.25;
        let b = -0.8;
        let score_coeffs = score_basis_cell_coefficients(score_basis_span, b);
        let link_coeffs = link_basis_cell_coefficients(link_basis_span, a, b);
        for &z in &[-0.7, -0.1, 0.2, 0.4] {
            let score_poly = polynomial_value(&score_coeffs, z);
            let link_poly = polynomial_value(&link_coeffs, z);
            assert!((score_poly - b * score_basis_span.evaluate(z)).abs() < 1e-12);
            assert!((link_poly - link_basis_span.evaluate(a + b * z)).abs() < 1e-12);
        }
    }

    #[test]
    fn link_basis_partials_match_exact_span_derivatives() {
        let link_basis_span = LocalSpanCubic {
            left: -0.5,
            right: 1.1,
            c0: -0.03,
            c1: 0.05,
            c2: -0.02,
            c3: 0.01,
        };
        let a = 0.25;
        let b = -0.8;
        let (dc_da, dc_db) = link_basis_cell_coefficient_partials(link_basis_span, a, b);
        let (dc_daa, dc_dab, dc_dbb) = link_basis_cell_second_partials(link_basis_span, a, b);
        for &z in &[-0.6, -0.2, 0.15, 0.5] {
            let u = a + b * z;
            let eta_a = link_basis_span.first_derivative(u);
            let eta_b = z * link_basis_span.first_derivative(u);
            let eta_aa = link_basis_span.second_derivative(u);
            let eta_ab = z * link_basis_span.second_derivative(u);
            let eta_bb = z * z * link_basis_span.second_derivative(u);
            assert!((polynomial_value(&dc_da, z) - eta_a).abs() < 1e-12);
            assert!((polynomial_value(&dc_db, z) - eta_b).abs() < 1e-12);
            assert!((polynomial_value(&dc_daa, z) - eta_aa).abs() < 1e-12);
            assert!((polynomial_value(&dc_dab, z) - eta_ab).abs() < 1e-12);
            assert!((polynomial_value(&dc_dbb, z) - eta_bb).abs() < 1e-12);
        }
    }

    #[test]
    fn denested_third_partials_match_exact_span_derivatives() {
        let link_span = LocalSpanCubic {
            left: -0.6,
            right: 0.9,
            c0: -0.05,
            c1: 0.04,
            c2: -0.02,
            c3: 0.015,
        };
        let (dc_daaa, dc_daab, dc_dabb, dc_dbbb) = denested_cell_third_partials(link_span);
        let link_third = 6.0 * link_span.c3;
        for &z in &[-0.75, -0.4, -0.1, 0.2] {
            let eta_aaa = link_third;
            let eta_aab = z * link_third;
            let eta_abb = z * z * link_third;
            let eta_bbb = z * z * z * link_third;
            assert!((polynomial_value(&dc_daaa, z) - eta_aaa).abs() < 1e-12);
            assert!((polynomial_value(&dc_daab, z) - eta_aab).abs() < 1e-12);
            assert!((polynomial_value(&dc_dabb, z) - eta_abb).abs() < 1e-12);
            assert!((polynomial_value(&dc_dbbb, z) - eta_bbb).abs() < 1e-12);
        }
    }

    #[test]
    fn link_basis_third_partials_match_exact_span_derivatives() {
        let link_basis_span = LocalSpanCubic {
            left: -0.5,
            right: 1.1,
            c0: -0.03,
            c1: 0.05,
            c2: -0.02,
            c3: 0.01,
        };
        let (dc_daaa, dc_daab, dc_dabb, dc_dbbb) = link_basis_cell_third_partials(link_basis_span);
        let link_third = 6.0 * link_basis_span.c3;
        for &z in &[-0.6, -0.2, 0.15, 0.5] {
            let eta_aaa = link_third;
            let eta_aab = z * link_third;
            let eta_abb = z * z * link_third;
            let eta_bbb = z * z * z * link_third;
            assert!((polynomial_value(&dc_daaa, z) - eta_aaa).abs() < 1e-12);
            assert!((polynomial_value(&dc_daab, z) - eta_aab).abs() < 1e-12);
            assert!((polynomial_value(&dc_dabb, z) - eta_abb).abs() < 1e-12);
            assert!((polynomial_value(&dc_dbbb, z) - eta_bbb).abs() < 1e-12);
        }
    }

    #[test]
    fn branch_selection_uses_normalized_non_affine_coefficients() {
        let affine = DenestedCubicCell {
            left: -1.0,
            right: 1.0,
            c0: 0.1,
            c1: -0.4,
            c2: 1e-13,
            c3: -1e-13,
        };
        let quartic = DenestedCubicCell {
            c2: 2e-4,
            c3: 1e-13,
            ..affine
        };
        let sextic = DenestedCubicCell {
            c2: 2e-4,
            c3: 5e-3,
            ..affine
        };
        assert_eq!(branch_cell(affine).unwrap(), ExactCellBranch::Affine);
        assert_eq!(branch_cell(quartic).unwrap(), ExactCellBranch::Quartic);
        assert_eq!(branch_cell(sextic).unwrap(), ExactCellBranch::Sextic);
    }

    #[test]
    fn affine_anchor_moments_match_whole_line_closed_forms() {
        let out = affine_anchor_moment_vector(0.0, 0.0, f64::NEG_INFINITY, f64::INFINITY, 4);
        // `affine_anchor_moment_vector` returns the RAW substrate moments
        // `T_n = ∫ z^n exp(-½z²) dz` (the cubic-cell `∫ z^n exp(-q) dz`
        // convention that every production consumer and the GPU parity path
        // share; the `1/√(2π)` is folded in downstream via `INV_TWO_PI`). At
        // the affine identity the anchor is the *unnormalized* standard normal,
        // so M0 = M2 = √(2π) and M1 = 0 — the normalized {1, 0, 1} moments
        // scaled by the whole-line mass √(2π).
        let sqrt_2pi = (2.0 * std::f64::consts::PI).sqrt();
        assert!((out[0] - sqrt_2pi).abs() < 1e-12);
        assert!(out[1].abs() < 1e-12);
        assert!((out[2] - sqrt_2pi).abs() < 1e-12);
    }

    #[test]
    fn affine_anchor_moments_match_shifted_gaussian_whole_line() {
        let alpha = 0.7;
        let beta = -0.4;
        let out = affine_anchor_moment_vector(alpha, beta, f64::NEG_INFINITY, f64::INFINITY, 4);
        let s = (1.0 + beta * beta).sqrt();
        let mu = -alpha * beta / (1.0 + beta * beta);
        // RAW (unnormalized) whole-line moments of the affine anchor
        // `exp(-½(alpha + beta·z)²)·exp(-½z²)`, an unnormalized Gaussian with
        // mean `mu` and variance `1/s²`. Its raw moments carry the `√(2π)` mass
        // factor: M0 = √(2π)·scale, M1 = √(2π)·scale·mu,
        // M2 = √(2π)·scale·(mu² + 1/s²), where the anchor amplitude
        // `scale = exp(-alpha² / 2s²) / s`.
        let scale = (-alpha * alpha / (2.0 * s * s)).exp() / s;
        let sqrt_2pi = (2.0 * std::f64::consts::PI).sqrt();
        assert!((out[0] - scale * sqrt_2pi).abs() < 1e-12);
        assert!((out[1] - scale * sqrt_2pi * mu).abs() < 1e-12);
        assert!((out[2] - scale * sqrt_2pi * (mu * mu + 1.0 / (s * s))).abs() < 1e-10);
    }

    #[test]
    fn quartic_recurrence_reduces_higher_moments() {
        let cell = DenestedCubicCell {
            left: -1.0,
            right: 0.9,
            c0: 0.2,
            c1: -0.3,
            c2: 0.18,
            c3: 0.0,
        };
        let exact = |k: usize| {
            simpson_integral(cell.left, cell.right, 2000, |z| {
                z.powi(k as i32) * (-cell.q(z)).exp()
            })
        };
        let reduced = reduce_quartic_moments(cell, [exact(0), exact(1), exact(2)], 6)
            .expect("quartic reduction");
        for k in 0..=6 {
            let target = exact(k);
            assert!(
                (reduced[k] - target).abs() < 1e-7,
                "quartic reduced moment M{k} mismatch: {} vs {}",
                reduced[k],
                target
            );
        }
    }

    #[test]
    fn sextic_recurrence_reduces_higher_moments() {
        let cell = DenestedCubicCell {
            left: -0.8,
            right: 0.7,
            c0: -0.1,
            c1: 0.25,
            c2: -0.14,
            c3: 0.22,
        };
        let exact = |k: usize| {
            simpson_integral(cell.left, cell.right, 3000, |z| {
                z.powi(k as i32) * (-cell.q(z)).exp()
            })
        };
        let reduced =
            reduce_sextic_moments(cell, [exact(0), exact(1), exact(2), exact(3), exact(4)], 9)
                .expect("sextic reduction");
        for k in 0..=9 {
            let target = exact(k);
            assert!(
                (reduced[k] - target).abs() < 1e-7,
                "sextic reduced moment M{k} mismatch: {} vs {}",
                reduced[k],
                target
            );
        }
    }

    #[test]
    fn degenerate_sextic_branch_preserves_quadratic_coefficient() {
        let cell = DenestedCubicCell {
            left: -1.0,
            right: 1.0,
            c0: 0.0,
            c1: 0.0,
            c2: 0.1,
            c3: 2.0e-10,
        };
        assert_eq!(branch_cell(cell).unwrap(), ExactCellBranch::Sextic);

        let state = evaluate_cell_moments(cell, 9).expect("degenerate sextic cell");
        let quartic_cell = DenestedCubicCell { c3: 0.0, ..cell };
        let quartic = evaluate_cell_moments(quartic_cell, 9).expect("quartic cell");
        let affine = evaluate_affine_cell_state(
            DenestedCubicCell {
                c2: 0.0,
                c3: 0.0,
                ..cell
            },
            9,
        )
        .expect("affine cell");

        assert_eq!(state.branch, ExactCellBranch::Quartic);
        for k in 0..=9 {
            assert!(
                (state.moments[k] - quartic.moments[k]).abs() < 1e-12,
                "lowered moment M{k} should match the quartic cell: {} vs {}",
                state.moments[k],
                quartic.moments[k]
            );
        }
        assert!(
            (state.moments[0] - affine.moments[0]).abs() > 1e-4,
            "degenerate sextic handling must not drop the nonzero c2 term"
        );
    }

    #[test]
    fn moment_reduced_first_and_second_derivatives_match_numeric_integrals() {
        let cell = DenestedCubicCell {
            left: -0.9,
            right: 0.6,
            c0: 0.15,
            c1: -0.2,
            c2: 0.08,
            c3: 0.17,
        };
        let moments = reduce_sextic_moments(
            cell,
            [
                simpson_integral(cell.left, cell.right, 3000, |z| (-cell.q(z)).exp()),
                simpson_integral(cell.left, cell.right, 3000, |z| z * (-cell.q(z)).exp()),
                simpson_integral(cell.left, cell.right, 3000, |z| z * z * (-cell.q(z)).exp()),
                simpson_integral(cell.left, cell.right, 3000, |z| {
                    z.powi(3) * (-cell.q(z)).exp()
                }),
                simpson_integral(cell.left, cell.right, 3000, |z| {
                    z.powi(4) * (-cell.q(z)).exp()
                }),
            ],
            9,
        )
        .expect("reduced moments");

        let r = [0.7, -0.1, 0.3];
        let s = [0.2, 0.5];
        let second = [0.4, -0.2, 0.1];
        let exact_first = cell_first_derivative_from_moments(&r, &moments).expect("first");
        let exact_second =
            cell_second_derivative_from_moments(cell, &r, &s, &second, &moments).expect("second");

        let numeric_first = simpson_integral(cell.left, cell.right, 3000, |z| {
            polynomial_value(&r, z) * (-cell.q(z)).exp() / (2.0 * std::f64::consts::PI)
        });
        let numeric_second = simpson_integral(cell.left, cell.right, 3000, |z| {
            let eta = cell.eta(z);
            (polynomial_value(&second, z) - eta * polynomial_value(&r, z) * polynomial_value(&s, z))
                * (-cell.q(z)).exp()
                / (2.0 * std::f64::consts::PI)
        });

        assert!((exact_first - numeric_first).abs() < 1e-7);
        assert!((exact_second - numeric_second).abs() < 1e-7);
    }

    #[test]
    fn moment_reduced_third_derivative_matches_numeric_integral() {
        let cell = DenestedCubicCell {
            left: -0.85,
            right: 0.7,
            c0: -0.12,
            c1: 0.18,
            c2: 0.09,
            c3: -0.11,
        };
        let moments = evaluate_cell_moments(cell, 12).expect("cell moments");
        let r = [0.35, -0.12, 0.08];
        let s = [0.17, 0.09];
        let t = [-0.21, 0.14, -0.04];
        let rs = [0.11, -0.07, 0.05];
        let rt = [-0.06, 0.03];
        let st = [0.08, -0.02, 0.01];
        let rst = [0.04, -0.05, 0.02];

        let exact_third = cell_third_derivative_from_moments(
            cell,
            &r,
            &s,
            &t,
            &rs,
            &rt,
            &st,
            &rst,
            &moments.moments,
        )
        .expect("third derivative");
        let numeric_third = simpson_integral(cell.left, cell.right, 4000, |z| {
            let eta = cell.eta(z);
            let rz = polynomial_value(&r, z);
            let sz = polynomial_value(&s, z);
            let tz = polynomial_value(&t, z);
            let rsz = polynomial_value(&rs, z);
            let rtz = polynomial_value(&rt, z);
            let stz = polynomial_value(&st, z);
            let rstz = polynomial_value(&rst, z);
            (rstz - eta * (rsz * tz + rtz * sz + stz * rz) + (eta * eta - 1.0) * rz * sz * tz)
                * (-cell.q(z)).exp()
                / (2.0 * std::f64::consts::PI)
        });

        assert!((exact_third - numeric_third).abs() < 1e-7);
    }

    #[test]
    fn moment_reduced_fourth_derivative_matches_numeric_integral() {
        let cell = DenestedCubicCell {
            left: -0.8,
            right: 0.65,
            c0: 0.11,
            c1: -0.22,
            c2: 0.07,
            c3: 0.13,
        };
        let moments = evaluate_cell_moments(cell, 16).expect("cell moments");
        let r = [0.21, -0.13, 0.06];
        let s = [-0.18, 0.04];
        let t = [0.09, 0.07, -0.03];
        let u = [-0.14, 0.05];
        let rs = [0.08, -0.03, 0.02];
        let rt = [-0.05, 0.01];
        let ru = [0.04, -0.02, 0.01];
        let st = [0.03, 0.02];
        let su = [-0.02, 0.05, -0.01];
        let tu = [0.07, -0.04];
        let rst = [0.03, -0.01, 0.02];
        let rsu = [-0.02, 0.04];
        let rtu = [0.01, 0.02, -0.01];
        let stu = [-0.03, 0.02];
        let rstu = [0.02, -0.01, 0.01];

        let exact_fourth = cell_fourth_derivative_from_moments(
            cell,
            &r,
            &s,
            &t,
            &u,
            &rs,
            &rt,
            &ru,
            &st,
            &su,
            &tu,
            &rst,
            &rsu,
            &rtu,
            &stu,
            &rstu,
            &moments.moments,
        )
        .expect("fourth derivative");
        let numeric_fourth = simpson_integral(cell.left, cell.right, 5000, |z| {
            let eta = cell.eta(z);
            let rz = polynomial_value(&r, z);
            let sz = polynomial_value(&s, z);
            let tz = polynomial_value(&t, z);
            let uz = polynomial_value(&u, z);
            let rsz = polynomial_value(&rs, z);
            let rtz = polynomial_value(&rt, z);
            let ruz = polynomial_value(&ru, z);
            let stz = polynomial_value(&st, z);
            let suz = polynomial_value(&su, z);
            let tuz = polynomial_value(&tu, z);
            let rstz = polynomial_value(&rst, z);
            let rsuz = polynomial_value(&rsu, z);
            let rtuz = polynomial_value(&rtu, z);
            let stuz = polynomial_value(&stu, z);
            let rstuz = polynomial_value(&rstu, z);
            let linear =
                rstz * uz + rsuz * tz + rtuz * sz + stuz * rz + rsz * tuz + rtz * suz + ruz * stz;
            let quadratic = rsz * tz * uz
                + rtz * sz * uz
                + ruz * sz * tz
                + stz * rz * uz
                + suz * rz * tz
                + tuz * rz * sz;
            let quartic = rz * sz * tz * uz;
            (rstuz - eta * linear
                + (eta * eta - 1.0) * quadratic
                + (-eta * eta * eta + 3.0 * eta) * quartic)
                * (-cell.q(z)).exp()
                / (2.0 * std::f64::consts::PI)
        });

        assert!((exact_fourth - numeric_fourth).abs() < 2e-7);
    }

    #[test]
    fn denested_cell_parameter_derivatives_match_exact_integrands() {
        let score_span = LocalSpanCubic {
            left: -0.75,
            right: 0.25,
            c0: 0.08,
            c1: -0.03,
            c2: 0.02,
            c3: -0.01,
        };
        let link_span = LocalSpanCubic {
            left: -0.6,
            right: 0.9,
            c0: -0.05,
            c1: 0.04,
            c2: -0.02,
            c3: 0.015,
        };
        let a = 0.3;
        let b = -0.7;
        let coeffs = denested_cell_coefficients(score_span, link_span, a, b);
        let cell = DenestedCubicCell {
            left: score_span.left,
            right: score_span.right,
            c0: coeffs[0],
            c1: coeffs[1],
            c2: coeffs[2],
            c3: coeffs[3],
        };
        let state = evaluate_cell_moments(cell, 24).expect("cell moments");
        let (dc_da, dc_db) = denested_cell_coefficient_partials(score_span, link_span, a, b);
        let (dc_daa, dc_dab, dc_dbb) = denested_cell_second_partials(score_span, link_span, a, b);
        let (dc_daaa, dc_daab, dc_dabb, dc_dbbb) = denested_cell_third_partials(link_span);
        let zero = [0.0; 4];
        let link_third = 6.0 * link_span.c3;

        let eta_a = |z: f64| 1.0 + link_span.first_derivative(a + b * z);
        let eta_b = |z: f64| z + score_span.evaluate(z) + z * link_span.first_derivative(a + b * z);
        let eta_aa = |z: f64| link_span.second_derivative(a + b * z);
        let eta_ab = |z: f64| z * link_span.second_derivative(a + b * z);
        let eta_bb = |z: f64| z * z * link_span.second_derivative(a + b * z);
        let eta_aaa = |z: f64| link_third + 0.0 * z;
        let eta_aab = |z: f64| z * link_third;
        let eta_abb = |z: f64| z * z * link_third;
        let eta_bbb = |z: f64| z * z * z * link_third;

        let exact_a = cell_first_derivative_from_moments(&dc_da, &state.moments).expect("a");
        let exact_b = cell_first_derivative_from_moments(&dc_db, &state.moments).expect("b");
        let exact_aa =
            cell_second_derivative_from_moments(cell, &dc_da, &dc_da, &dc_daa, &state.moments)
                .expect("aa");
        let exact_ab =
            cell_second_derivative_from_moments(cell, &dc_da, &dc_db, &dc_dab, &state.moments)
                .expect("ab");
        let exact_bb =
            cell_second_derivative_from_moments(cell, &dc_db, &dc_db, &dc_dbb, &state.moments)
                .expect("bb");
        let exact_aaa = cell_third_derivative_from_moments(
            cell,
            &dc_da,
            &dc_da,
            &dc_da,
            &dc_daa,
            &dc_daa,
            &dc_daa,
            &dc_daaa,
            &state.moments,
        )
        .expect("aaa");
        let exact_aab = cell_third_derivative_from_moments(
            cell,
            &dc_da,
            &dc_da,
            &dc_db,
            &dc_daa,
            &dc_dab,
            &dc_dab,
            &dc_daab,
            &state.moments,
        )
        .expect("aab");
        let exact_abb = cell_third_derivative_from_moments(
            cell,
            &dc_da,
            &dc_db,
            &dc_db,
            &dc_dab,
            &dc_dab,
            &dc_dbb,
            &dc_dabb,
            &state.moments,
        )
        .expect("abb");
        let exact_bbb = cell_third_derivative_from_moments(
            cell,
            &dc_db,
            &dc_db,
            &dc_db,
            &dc_dbb,
            &dc_dbb,
            &dc_dbb,
            &dc_dbbb,
            &state.moments,
        )
        .expect("bbb");
        let exact_aaaa = cell_fourth_derivative_from_moments(
            cell,
            &dc_da,
            &dc_da,
            &dc_da,
            &dc_da,
            &dc_daa,
            &dc_daa,
            &dc_daa,
            &dc_daa,
            &dc_daa,
            &dc_daa,
            &dc_daaa,
            &dc_daaa,
            &dc_daaa,
            &dc_daaa,
            &zero,
            &state.moments,
        )
        .expect("aaaa");
        let exact_aaab = cell_fourth_derivative_from_moments(
            cell,
            &dc_da,
            &dc_da,
            &dc_da,
            &dc_db,
            &dc_daa,
            &dc_daa,
            &dc_dab,
            &dc_daa,
            &dc_dab,
            &dc_dab,
            &dc_daaa,
            &dc_daab,
            &dc_daab,
            &dc_daab,
            &zero,
            &state.moments,
        )
        .expect("aaab");
        let exact_aabb = cell_fourth_derivative_from_moments(
            cell,
            &dc_da,
            &dc_da,
            &dc_db,
            &dc_db,
            &dc_daa,
            &dc_dab,
            &dc_dab,
            &dc_dab,
            &dc_dab,
            &dc_dbb,
            &dc_daab,
            &dc_daab,
            &dc_dabb,
            &dc_dabb,
            &zero,
            &state.moments,
        )
        .expect("aabb");
        let exact_abbb = cell_fourth_derivative_from_moments(
            cell,
            &dc_da,
            &dc_db,
            &dc_db,
            &dc_db,
            &dc_dab,
            &dc_dab,
            &dc_dab,
            &dc_dbb,
            &dc_dbb,
            &dc_dbb,
            &dc_dabb,
            &dc_dabb,
            &dc_dabb,
            &dc_dbbb,
            &zero,
            &state.moments,
        )
        .expect("abbb");
        let exact_bbbb = cell_fourth_derivative_from_moments(
            cell,
            &dc_db,
            &dc_db,
            &dc_db,
            &dc_db,
            &dc_dbb,
            &dc_dbb,
            &dc_dbb,
            &dc_dbb,
            &dc_dbb,
            &dc_dbb,
            &dc_dbbb,
            &dc_dbbb,
            &dc_dbbb,
            &dc_dbbb,
            &zero,
            &state.moments,
        )
        .expect("bbbb");

        let numeric_a = simpson_integral(cell.left, cell.right, 5000, |z| {
            eta_a(z) * (-cell.q(z)).exp() * INV_TWO_PI
        });
        let numeric_b = simpson_integral(cell.left, cell.right, 5000, |z| {
            eta_b(z) * (-cell.q(z)).exp() * INV_TWO_PI
        });
        let numeric_aa = simpson_integral(cell.left, cell.right, 5000, |z| {
            (eta_aa(z) - cell.eta(z) * eta_a(z) * eta_a(z)) * (-cell.q(z)).exp() * INV_TWO_PI
        });
        let numeric_ab = simpson_integral(cell.left, cell.right, 5000, |z| {
            (eta_ab(z) - cell.eta(z) * eta_a(z) * eta_b(z)) * (-cell.q(z)).exp() * INV_TWO_PI
        });
        let numeric_bb = simpson_integral(cell.left, cell.right, 5000, |z| {
            (eta_bb(z) - cell.eta(z) * eta_b(z) * eta_b(z)) * (-cell.q(z)).exp() * INV_TWO_PI
        });
        let numeric_aaa = simpson_integral(cell.left, cell.right, 5000, |z| {
            let eta = cell.eta(z);
            (eta_aaa(z) - 3.0 * eta * eta_aa(z) * eta_a(z) + (eta * eta - 1.0) * eta_a(z).powi(3))
                * (-cell.q(z)).exp()
                * INV_TWO_PI
        });
        let numeric_aab = simpson_integral(cell.left, cell.right, 5000, |z| {
            let eta = cell.eta(z);
            let a_z = eta_a(z);
            let b_z = eta_b(z);
            (eta_aab(z) - eta * (eta_aa(z) * b_z + 2.0 * eta_ab(z) * a_z)
                + (eta * eta - 1.0) * a_z * a_z * b_z)
                * (-cell.q(z)).exp()
                * INV_TWO_PI
        });
        let numeric_abb = simpson_integral(cell.left, cell.right, 5000, |z| {
            let eta = cell.eta(z);
            let a_z = eta_a(z);
            let b_z = eta_b(z);
            (eta_abb(z) - eta * (2.0 * eta_ab(z) * b_z + eta_bb(z) * a_z)
                + (eta * eta - 1.0) * a_z * b_z * b_z)
                * (-cell.q(z)).exp()
                * INV_TWO_PI
        });
        let numeric_bbb = simpson_integral(cell.left, cell.right, 5000, |z| {
            let eta = cell.eta(z);
            (eta_bbb(z) - 3.0 * eta * eta_bb(z) * eta_b(z) + (eta * eta - 1.0) * eta_b(z).powi(3))
                * (-cell.q(z)).exp()
                * INV_TWO_PI
        });
        let numeric_aaaa = simpson_integral(cell.left, cell.right, 5000, |z| {
            let eta = cell.eta(z);
            let eta_a_z = eta_a(z);
            let eta_aa_z = eta_aa(z);
            let eta_aaa_z = eta_aaa(z);
            (-eta * (4.0 * eta_aaa_z * eta_a_z + 3.0 * eta_aa_z * eta_aa_z)
                + (eta * eta - 1.0) * (6.0 * eta_aa_z * eta_a_z * eta_a_z)
                + (-eta * eta * eta + 3.0 * eta) * eta_a_z.powi(4))
                * (-cell.q(z)).exp()
                * INV_TWO_PI
        });
        let numeric_aaab = simpson_integral(cell.left, cell.right, 5000, |z| {
            let eta = cell.eta(z);
            let a_z = eta_a(z);
            let b_z = eta_b(z);
            let aa_z = eta_aa(z);
            let ab_z = eta_ab(z);
            let aaa_z = eta_aaa(z);
            let aab_z = eta_aab(z);
            (-eta * (aaa_z * b_z + 3.0 * aab_z * a_z + 3.0 * aa_z * ab_z)
                + (eta * eta - 1.0) * (3.0 * aa_z * a_z * b_z + 3.0 * ab_z * a_z * a_z)
                + (-eta * eta * eta + 3.0 * eta) * a_z.powi(3) * b_z)
                * (-cell.q(z)).exp()
                * INV_TWO_PI
        });
        let numeric_aabb = simpson_integral(cell.left, cell.right, 5000, |z| {
            let eta = cell.eta(z);
            let a_z = eta_a(z);
            let b_z = eta_b(z);
            let aa_z = eta_aa(z);
            let ab_z = eta_ab(z);
            let bb_z = eta_bb(z);
            let aab_z = eta_aab(z);
            let abb_z = eta_abb(z);
            (-eta * (2.0 * aab_z * b_z + 2.0 * abb_z * a_z + aa_z * bb_z + 2.0 * ab_z * ab_z)
                + (eta * eta - 1.0)
                    * (aa_z * b_z * b_z + 4.0 * ab_z * a_z * b_z + bb_z * a_z * a_z)
                + (-eta * eta * eta + 3.0 * eta) * a_z * a_z * b_z * b_z)
                * (-cell.q(z)).exp()
                * INV_TWO_PI
        });
        let numeric_abbb = simpson_integral(cell.left, cell.right, 5000, |z| {
            let eta = cell.eta(z);
            let a_z = eta_a(z);
            let b_z = eta_b(z);
            let ab_z = eta_ab(z);
            let bb_z = eta_bb(z);
            let abb_z = eta_abb(z);
            let bbb_z = eta_bbb(z);
            (-eta * (3.0 * abb_z * b_z + bbb_z * a_z + 3.0 * ab_z * bb_z)
                + (eta * eta - 1.0) * (3.0 * ab_z * b_z * b_z + 3.0 * bb_z * a_z * b_z)
                + (-eta * eta * eta + 3.0 * eta) * a_z * b_z.powi(3))
                * (-cell.q(z)).exp()
                * INV_TWO_PI
        });
        let numeric_bbbb = simpson_integral(cell.left, cell.right, 5000, |z| {
            let eta = cell.eta(z);
            let eta_b_z = eta_b(z);
            let eta_bb_z = eta_bb(z);
            let eta_bbb_z = eta_bbb(z);
            (-eta * (4.0 * eta_bbb_z * eta_b_z + 3.0 * eta_bb_z * eta_bb_z)
                + (eta * eta - 1.0) * (6.0 * eta_bb_z * eta_b_z * eta_b_z)
                + (-eta * eta * eta + 3.0 * eta) * eta_b_z.powi(4))
                * (-cell.q(z)).exp()
                * INV_TWO_PI
        });

        assert!((exact_a - numeric_a).abs() < 1e-8);
        assert!((exact_b - numeric_b).abs() < 1e-8);
        assert!((exact_aa - numeric_aa).abs() < 1e-8);
        assert!((exact_ab - numeric_ab).abs() < 1e-8);
        assert!((exact_bb - numeric_bb).abs() < 1e-8);
        assert!((exact_aaa - numeric_aaa).abs() < 2e-7);
        assert!((exact_aab - numeric_aab).abs() < 2e-7);
        assert!((exact_abb - numeric_abb).abs() < 2e-7);
        assert!((exact_bbb - numeric_bbb).abs() < 2e-7);
        assert!((exact_aaaa - numeric_aaaa).abs() < 2e-6);
        assert!((exact_aaab - numeric_aaab).abs() < 2e-6);
        assert!((exact_aabb - numeric_aabb).abs() < 2e-6);
        assert!((exact_abbb - numeric_abbb).abs() < 2e-6);
        assert!((exact_bbbb - numeric_bbbb).abs() < 2e-6);
    }

    #[test]
    fn link_basis_cell_derivatives_match_exact_integrands() {
        let score_span = LocalSpanCubic {
            left: -0.75,
            right: 0.25,
            c0: 0.08,
            c1: -0.03,
            c2: 0.02,
            c3: -0.01,
        };
        let link_span = LocalSpanCubic {
            left: -0.6,
            right: 0.9,
            c0: -0.05,
            c1: 0.04,
            c2: -0.02,
            c3: 0.015,
        };
        let link_basis_span = LocalSpanCubic {
            left: -0.6,
            right: 0.9,
            c0: 0.02,
            c1: -0.01,
            c2: 0.03,
            c3: -0.02,
        };
        let a = 0.3;
        let b = -0.7;
        let coeffs = denested_cell_coefficients(score_span, link_span, a, b);
        let cell = DenestedCubicCell {
            left: score_span.left,
            right: score_span.right,
            c0: coeffs[0],
            c1: coeffs[1],
            c2: coeffs[2],
            c3: coeffs[3],
        };
        let state = evaluate_cell_moments(cell, 24).expect("cell moments");
        let (dc_da, dc_db) = denested_cell_coefficient_partials(score_span, link_span, a, b);
        let second_partials = denested_cell_second_partials(score_span, link_span, a, b);
        let dc_daa = second_partials.0;
        let dc_dab = second_partials.1;
        let dc_dbb = second_partials.2;
        let denested_third = denested_cell_third_partials(link_span);
        let dc_daaa = denested_third.0;
        let dc_dbbb = denested_third.3;

        let coeff_w = link_basis_cell_coefficients(link_basis_span, a, b);
        let (coeff_aw, coeff_bw) = link_basis_cell_coefficient_partials(link_basis_span, a, b);
        let (coeff_aaw, coeff_abw, coeff_bbw) =
            link_basis_cell_second_partials(link_basis_span, a, b);
        let link_basis_third = link_basis_cell_third_partials(link_basis_span);
        let coeff_aaaw = link_basis_third.0;
        let coeff_bbbw = link_basis_third.3;
        let zero = [0.0; 4];
        let basis_third = 6.0 * link_basis_span.c3;

        let eta_a = |z: f64| 1.0 + link_span.first_derivative(a + b * z);
        let eta_b = |z: f64| z + score_span.evaluate(z) + z * link_span.first_derivative(a + b * z);
        let eta_aa = |z: f64| link_span.second_derivative(a + b * z);
        let eta_ab = |z: f64| z * link_span.second_derivative(a + b * z);
        let eta_bb = |z: f64| z * z * link_span.second_derivative(a + b * z);
        let eta_w = |z: f64| link_basis_span.evaluate(a + b * z);
        let eta_aw = |z: f64| link_basis_span.first_derivative(a + b * z);
        let eta_bw = |z: f64| z * link_basis_span.first_derivative(a + b * z);
        let eta_aaw = |z: f64| link_basis_span.second_derivative(a + b * z);
        let eta_abw = |z: f64| z * link_basis_span.second_derivative(a + b * z);
        let eta_bbw = |z: f64| z * z * link_basis_span.second_derivative(a + b * z);
        let eta_aaaw = |z: f64| basis_third + 0.0 * z;
        let eta_bbbw = |z: f64| z * z * z * basis_third;

        let exact_w = cell_first_derivative_from_moments(&coeff_w, &state.moments).expect("w");
        let exact_aw =
            cell_second_derivative_from_moments(cell, &dc_da, &coeff_w, &coeff_aw, &state.moments)
                .expect("aw");
        let exact_bw =
            cell_second_derivative_from_moments(cell, &dc_db, &coeff_w, &coeff_bw, &state.moments)
                .expect("bw");
        let exact_ww =
            cell_second_derivative_from_moments(cell, &coeff_w, &coeff_w, &zero, &state.moments)
                .expect("ww");
        let exact_aaw = cell_third_derivative_from_moments(
            cell,
            &dc_da,
            &dc_da,
            &coeff_w,
            &dc_daa,
            &coeff_aw,
            &coeff_aw,
            &coeff_aaw,
            &state.moments,
        )
        .expect("aaw");
        let exact_abw = cell_third_derivative_from_moments(
            cell,
            &dc_da,
            &dc_db,
            &coeff_w,
            &dc_dab,
            &coeff_aw,
            &coeff_bw,
            &coeff_abw,
            &state.moments,
        )
        .expect("abw");
        let exact_bbw = cell_third_derivative_from_moments(
            cell,
            &dc_db,
            &dc_db,
            &coeff_w,
            &dc_dbb,
            &coeff_bw,
            &coeff_bw,
            &coeff_bbw,
            &state.moments,
        )
        .expect("bbw");
        let exact_www = cell_third_derivative_from_moments(
            cell,
            &coeff_w,
            &coeff_w,
            &coeff_w,
            &zero,
            &zero,
            &zero,
            &zero,
            &state.moments,
        )
        .expect("www");
        let exact_aaaw = cell_fourth_derivative_from_moments(
            cell,
            &dc_da,
            &dc_da,
            &dc_da,
            &coeff_w,
            &dc_daa,
            &dc_daa,
            &coeff_aw,
            &dc_daa,
            &coeff_aw,
            &coeff_aw,
            &dc_daaa,
            &coeff_aaw,
            &coeff_aaw,
            &coeff_aaw,
            &coeff_aaaw,
            &state.moments,
        )
        .expect("aaaw");
        let exact_aaww = cell_fourth_derivative_from_moments(
            cell,
            &dc_da,
            &dc_da,
            &coeff_w,
            &coeff_w,
            &dc_daa,
            &coeff_aw,
            &coeff_aw,
            &coeff_aw,
            &coeff_aw,
            &zero,
            &coeff_aaw,
            &coeff_aaw,
            &zero,
            &zero,
            &zero,
            &state.moments,
        )
        .expect("aaww");
        let exact_abww = cell_fourth_derivative_from_moments(
            cell,
            &dc_da,
            &dc_db,
            &coeff_w,
            &coeff_w,
            &dc_dab,
            &coeff_aw,
            &coeff_aw,
            &coeff_bw,
            &coeff_bw,
            &zero,
            &coeff_abw,
            &coeff_abw,
            &zero,
            &zero,
            &zero,
            &state.moments,
        )
        .expect("abww");
        let exact_bbww = cell_fourth_derivative_from_moments(
            cell,
            &dc_db,
            &dc_db,
            &coeff_w,
            &coeff_w,
            &dc_dbb,
            &coeff_bw,
            &coeff_bw,
            &coeff_bw,
            &coeff_bw,
            &zero,
            &coeff_bbw,
            &coeff_bbw,
            &zero,
            &zero,
            &zero,
            &state.moments,
        )
        .expect("bbww");
        let exact_bbbw = cell_fourth_derivative_from_moments(
            cell,
            &dc_db,
            &dc_db,
            &dc_db,
            &coeff_w,
            &dc_dbb,
            &dc_dbb,
            &coeff_bw,
            &dc_dbb,
            &coeff_bw,
            &coeff_bw,
            &dc_dbbb,
            &coeff_bbw,
            &coeff_bbw,
            &coeff_bbw,
            &coeff_bbbw,
            &state.moments,
        )
        .expect("bbbw");
        let exact_wwww = cell_fourth_derivative_from_moments(
            cell,
            &coeff_w,
            &coeff_w,
            &coeff_w,
            &coeff_w,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &state.moments,
        )
        .expect("wwww");

        let numeric_w = simpson_integral(cell.left, cell.right, 5000, |z| {
            eta_w(z) * (-cell.q(z)).exp() * INV_TWO_PI
        });
        let numeric_aw = simpson_integral(cell.left, cell.right, 5000, |z| {
            (eta_aw(z) - cell.eta(z) * eta_a(z) * eta_w(z)) * (-cell.q(z)).exp() * INV_TWO_PI
        });
        let numeric_bw = simpson_integral(cell.left, cell.right, 5000, |z| {
            (eta_bw(z) - cell.eta(z) * eta_b(z) * eta_w(z)) * (-cell.q(z)).exp() * INV_TWO_PI
        });
        let numeric_ww = simpson_integral(cell.left, cell.right, 5000, |z| {
            (-cell.eta(z) * eta_w(z) * eta_w(z)) * (-cell.q(z)).exp() * INV_TWO_PI
        });
        let numeric_aaw = simpson_integral(cell.left, cell.right, 5000, |z| {
            let eta = cell.eta(z);
            let w_z = eta_w(z);
            let a_z = eta_a(z);
            (eta_aaw(z) - eta * (eta_aa(z) * w_z + 2.0 * eta_aw(z) * a_z)
                + (eta * eta - 1.0) * a_z * a_z * w_z)
                * (-cell.q(z)).exp()
                * INV_TWO_PI
        });
        let numeric_abw = simpson_integral(cell.left, cell.right, 5000, |z| {
            let eta = cell.eta(z);
            let w_z = eta_w(z);
            let a_z = eta_a(z);
            let b_z = eta_b(z);
            (eta_abw(z) - eta * (eta_ab(z) * w_z + eta_aw(z) * b_z + eta_bw(z) * a_z)
                + (eta * eta - 1.0) * a_z * b_z * w_z)
                * (-cell.q(z)).exp()
                * INV_TWO_PI
        });
        let numeric_bbw = simpson_integral(cell.left, cell.right, 5000, |z| {
            let eta = cell.eta(z);
            let w_z = eta_w(z);
            let b_z = eta_b(z);
            (eta_bbw(z) - eta * (eta_bb(z) * w_z + 2.0 * eta_bw(z) * b_z)
                + (eta * eta - 1.0) * b_z * b_z * w_z)
                * (-cell.q(z)).exp()
                * INV_TWO_PI
        });
        let numeric_www = simpson_integral(cell.left, cell.right, 5000, |z| {
            let eta = cell.eta(z);
            let w_z = eta_w(z);
            ((eta * eta - 1.0) * w_z * w_z * w_z) * (-cell.q(z)).exp() * INV_TWO_PI
        });
        let numeric_aaaw = simpson_integral(cell.left, cell.right, 5000, |z| {
            let eta = cell.eta(z);
            let a_z = eta_a(z);
            let w_z = eta_w(z);
            let aa_z = eta_aa(z);
            let aw_z = eta_aw(z);
            (eta_aaaw(z)
                - eta * ((dc_daaa[0] + 0.0 * z) * w_z + 3.0 * eta_aaw(z) * a_z + 3.0 * aa_z * aw_z)
                + (eta * eta - 1.0) * (3.0 * aa_z * a_z * w_z + 3.0 * aw_z * a_z * a_z)
                + (-eta * eta * eta + 3.0 * eta) * a_z * a_z * a_z * w_z)
                * (-cell.q(z)).exp()
                * INV_TWO_PI
        });
        let numeric_aaww = simpson_integral(cell.left, cell.right, 5000, |z| {
            let eta = cell.eta(z);
            let a_z = eta_a(z);
            let w_z = eta_w(z);
            let aw_z = eta_aw(z);
            (-(2.0 * eta * (eta_aaw(z) * w_z + aw_z * aw_z))
                + (eta * eta - 1.0) * (eta_aa(z) * w_z * w_z + 4.0 * aw_z * a_z * w_z)
                + (-eta * eta * eta + 3.0 * eta) * a_z * a_z * w_z * w_z)
                * (-cell.q(z)).exp()
                * INV_TWO_PI
        });
        let numeric_abww = simpson_integral(cell.left, cell.right, 5000, |z| {
            let eta = cell.eta(z);
            let a_z = eta_a(z);
            let b_z = eta_b(z);
            let w_z = eta_w(z);
            let aw_z = eta_aw(z);
            let bw_z = eta_bw(z);
            (-(2.0 * eta * (eta_abw(z) * w_z + aw_z * bw_z))
                + (eta * eta - 1.0)
                    * (eta_ab(z) * w_z * w_z + 2.0 * aw_z * b_z * w_z + 2.0 * bw_z * a_z * w_z)
                + (-eta * eta * eta + 3.0 * eta) * a_z * b_z * w_z * w_z)
                * (-cell.q(z)).exp()
                * INV_TWO_PI
        });
        let numeric_bbww = simpson_integral(cell.left, cell.right, 5000, |z| {
            let eta = cell.eta(z);
            let b_z = eta_b(z);
            let w_z = eta_w(z);
            let bw_z = eta_bw(z);
            (-(2.0 * eta * (eta_bbw(z) * w_z + bw_z * bw_z))
                + (eta * eta - 1.0) * (eta_bb(z) * w_z * w_z + 4.0 * bw_z * b_z * w_z)
                + (-eta * eta * eta + 3.0 * eta) * b_z * b_z * w_z * w_z)
                * (-cell.q(z)).exp()
                * INV_TWO_PI
        });
        let numeric_bbbw = simpson_integral(cell.left, cell.right, 5000, |z| {
            let eta = cell.eta(z);
            let b_z = eta_b(z);
            let w_z = eta_w(z);
            let bb_z = eta_bb(z);
            let bw_z = eta_bw(z);
            (eta_bbbw(z)
                - eta
                    * ((dc_dbbb[3] * z * z * z) * w_z + 3.0 * eta_bbw(z) * b_z + 3.0 * bb_z * bw_z)
                + (eta * eta - 1.0) * (3.0 * bb_z * b_z * w_z + 3.0 * bw_z * b_z * b_z)
                + (-eta * eta * eta + 3.0 * eta) * b_z * b_z * b_z * w_z)
                * (-cell.q(z)).exp()
                * INV_TWO_PI
        });
        let numeric_wwww = simpson_integral(cell.left, cell.right, 5000, |z| {
            let eta = cell.eta(z);
            let w_z = eta_w(z);
            ((-eta * eta * eta + 3.0 * eta) * w_z * w_z * w_z * w_z)
                * (-cell.q(z)).exp()
                * INV_TWO_PI
        });

        assert!((exact_w - numeric_w).abs() < 1e-8);
        assert!((exact_aw - numeric_aw).abs() < 1e-7);
        assert!((exact_bw - numeric_bw).abs() < 1e-7);
        assert!((exact_ww - numeric_ww).abs() < 1e-7);
        assert!((exact_aaw - numeric_aaw).abs() < 2e-6);
        assert!((exact_abw - numeric_abw).abs() < 2e-6);
        assert!((exact_bbw - numeric_bbw).abs() < 2e-6);
        assert!((exact_www - numeric_www).abs() < 2e-6);
        assert!((exact_aaaw - numeric_aaaw).abs() < 3e-6);
        assert!((exact_aaww - numeric_aaww).abs() < 3e-6);
        assert!((exact_abww - numeric_abww).abs() < 3e-6);
        assert!((exact_bbww - numeric_bbww).abs() < 3e-6);
        assert!((exact_bbbw - numeric_bbbw).abs() < 3e-6);
        assert!((exact_wwww - numeric_wwww).abs() < 3e-6);
    }

    #[test]
    fn score_basis_cell_derivatives_match_exact_integrands() {
        let score_span = LocalSpanCubic {
            left: -0.75,
            right: 0.25,
            c0: 0.08,
            c1: -0.03,
            c2: 0.02,
            c3: -0.01,
        };
        let score_basis_span = LocalSpanCubic {
            left: -0.75,
            right: 0.25,
            c0: -0.04,
            c1: 0.06,
            c2: -0.01,
            c3: 0.02,
        };
        let link_span = LocalSpanCubic {
            left: -0.6,
            right: 0.9,
            c0: -0.05,
            c1: 0.04,
            c2: -0.02,
            c3: 0.015,
        };
        let a = 0.3;
        let b = -0.7;
        let coeffs = denested_cell_coefficients(score_span, link_span, a, b);
        let cell = DenestedCubicCell {
            left: score_span.left,
            right: score_span.right,
            c0: coeffs[0],
            c1: coeffs[1],
            c2: coeffs[2],
            c3: coeffs[3],
        };
        let state = evaluate_cell_moments(cell, 24).expect("cell moments");
        let (dc_da, dc_db) = denested_cell_coefficient_partials(score_span, link_span, a, b);
        let second_partials = denested_cell_second_partials(score_span, link_span, a, b);
        let dc_daa = second_partials.0;
        let dc_dab = second_partials.1;
        let dc_dbb = second_partials.2;
        let denested_third = denested_cell_third_partials(link_span);
        let dc_dbbb = denested_third.3;

        let coeff_h = score_basis_cell_coefficients(score_basis_span, b);
        let coeff_bh = score_basis_cell_coefficients(score_basis_span, 1.0);
        let zero = [0.0; 4];

        let eta_a = |z: f64| 1.0 + link_span.first_derivative(a + b * z);
        let eta_b = |z: f64| z + score_span.evaluate(z) + z * link_span.first_derivative(a + b * z);
        let eta_ab = |z: f64| z * link_span.second_derivative(a + b * z);
        let eta_bb = |z: f64| z * z * link_span.second_derivative(a + b * z);
        let eta_h = |z: f64| b * score_basis_span.evaluate(z);
        let eta_bh = |z: f64| score_basis_span.evaluate(z);

        let exact_h = cell_first_derivative_from_moments(&coeff_h, &state.moments).expect("h");
        let exact_ah =
            cell_second_derivative_from_moments(cell, &dc_da, &coeff_h, &zero, &state.moments)
                .expect("ah");
        let exact_bh =
            cell_second_derivative_from_moments(cell, &dc_db, &coeff_h, &coeff_bh, &state.moments)
                .expect("bh");
        let exact_hh =
            cell_second_derivative_from_moments(cell, &coeff_h, &coeff_h, &zero, &state.moments)
                .expect("hh");
        let exact_abh = cell_third_derivative_from_moments(
            cell,
            &dc_da,
            &dc_db,
            &coeff_h,
            &dc_dab,
            &zero,
            &coeff_bh,
            &zero,
            &state.moments,
        )
        .expect("abh");
        let exact_bbh = cell_third_derivative_from_moments(
            cell,
            &dc_db,
            &dc_db,
            &coeff_h,
            &dc_dbb,
            &coeff_bh,
            &coeff_bh,
            &zero,
            &state.moments,
        )
        .expect("bbh");
        let exact_bhh = cell_third_derivative_from_moments(
            cell,
            &dc_db,
            &coeff_h,
            &coeff_h,
            &coeff_bh,
            &coeff_bh,
            &zero,
            &zero,
            &state.moments,
        )
        .expect("bhh");
        let exact_hhh = cell_third_derivative_from_moments(
            cell,
            &coeff_h,
            &coeff_h,
            &coeff_h,
            &zero,
            &zero,
            &zero,
            &zero,
            &state.moments,
        )
        .expect("hhh");
        let exact_bbbh = cell_fourth_derivative_from_moments(
            cell,
            &dc_db,
            &dc_db,
            &dc_db,
            &coeff_h,
            &dc_dbb,
            &dc_dbb,
            &coeff_bh,
            &dc_dbb,
            &coeff_bh,
            &coeff_bh,
            &dc_dbbb,
            &zero,
            &zero,
            &zero,
            &zero,
            &state.moments,
        )
        .expect("bbbh");
        let exact_aahh = cell_fourth_derivative_from_moments(
            cell,
            &dc_da,
            &dc_da,
            &coeff_h,
            &coeff_h,
            &dc_daa,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &state.moments,
        )
        .expect("aahh");
        let exact_abhh = cell_fourth_derivative_from_moments(
            cell,
            &dc_da,
            &dc_db,
            &coeff_h,
            &coeff_h,
            &dc_dab,
            &zero,
            &zero,
            &coeff_bh,
            &coeff_bh,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &state.moments,
        )
        .expect("abhh");
        let exact_bbhh = cell_fourth_derivative_from_moments(
            cell,
            &dc_db,
            &dc_db,
            &coeff_h,
            &coeff_h,
            &dc_dbb,
            &coeff_bh,
            &coeff_bh,
            &coeff_bh,
            &coeff_bh,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &state.moments,
        )
        .expect("bbhh");
        let exact_bhhh = cell_fourth_derivative_from_moments(
            cell,
            &dc_db,
            &coeff_h,
            &coeff_h,
            &coeff_h,
            &coeff_bh,
            &coeff_bh,
            &coeff_bh,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &state.moments,
        )
        .expect("bhhh");
        let exact_hhhh = cell_fourth_derivative_from_moments(
            cell,
            &coeff_h,
            &coeff_h,
            &coeff_h,
            &coeff_h,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &state.moments,
        )
        .expect("hhhh");

        let numeric_h = simpson_integral(cell.left, cell.right, 5000, |z| {
            eta_h(z) * (-cell.q(z)).exp() * INV_TWO_PI
        });
        let numeric_ah = simpson_integral(cell.left, cell.right, 5000, |z| {
            (-cell.eta(z) * eta_a(z) * eta_h(z)) * (-cell.q(z)).exp() * INV_TWO_PI
        });
        let numeric_bh = simpson_integral(cell.left, cell.right, 5000, |z| {
            (eta_bh(z) - cell.eta(z) * eta_b(z) * eta_h(z)) * (-cell.q(z)).exp() * INV_TWO_PI
        });
        let numeric_hh = simpson_integral(cell.left, cell.right, 5000, |z| {
            (-cell.eta(z) * eta_h(z) * eta_h(z)) * (-cell.q(z)).exp() * INV_TWO_PI
        });
        let numeric_abh = simpson_integral(cell.left, cell.right, 5000, |z| {
            let eta = cell.eta(z);
            (-(eta * (eta_ab(z) * eta_h(z) + eta_bh(z) * eta_a(z)))
                + (eta * eta - 1.0) * eta_a(z) * eta_b(z) * eta_h(z))
                * (-cell.q(z)).exp()
                * INV_TWO_PI
        });
        let numeric_bbh = simpson_integral(cell.left, cell.right, 5000, |z| {
            let eta = cell.eta(z);
            (-(eta * (eta_bb(z) * eta_h(z) + 2.0 * eta_bh(z) * eta_b(z)))
                + (eta * eta - 1.0) * eta_b(z) * eta_b(z) * eta_h(z))
                * (-cell.q(z)).exp()
                * INV_TWO_PI
        });
        let numeric_bhh = simpson_integral(cell.left, cell.right, 5000, |z| {
            let eta = cell.eta(z);
            (-(2.0 * eta * eta_bh(z) * eta_h(z))
                + (eta * eta - 1.0) * eta_b(z) * eta_h(z) * eta_h(z))
                * (-cell.q(z)).exp()
                * INV_TWO_PI
        });
        let numeric_hhh = simpson_integral(cell.left, cell.right, 5000, |z| {
            let eta = cell.eta(z);
            ((eta * eta - 1.0) * eta_h(z) * eta_h(z) * eta_h(z)) * (-cell.q(z)).exp() * INV_TWO_PI
        });
        let numeric_bbbh = simpson_integral(cell.left, cell.right, 5000, |z| {
            let eta = cell.eta(z);
            let b_z = eta_b(z);
            let h_z = eta_h(z);
            let bb_z = eta_bb(z);
            let bh_z = eta_bh(z);
            (-(eta * ((dc_dbbb[3] * z * z * z) * h_z + 3.0 * bb_z * bh_z))
                + (eta * eta - 1.0) * (3.0 * bb_z * b_z * h_z + 3.0 * bh_z * b_z * b_z)
                + (-eta * eta * eta + 3.0 * eta) * b_z * b_z * b_z * h_z)
                * (-cell.q(z)).exp()
                * INV_TWO_PI
        });
        let numeric_aahh = simpson_integral(cell.left, cell.right, 5000, |z| {
            let eta = cell.eta(z);
            let a_z = eta_a(z);
            let h_z = eta_h(z);
            ((eta * eta - 1.0) * polynomial_value(&dc_daa, z) * h_z * h_z
                + (-eta * eta * eta + 3.0 * eta) * a_z * a_z * h_z * h_z)
                * (-cell.q(z)).exp()
                * INV_TWO_PI
        });
        let numeric_abhh = simpson_integral(cell.left, cell.right, 5000, |z| {
            let eta = cell.eta(z);
            let a_z = eta_a(z);
            let b_z = eta_b(z);
            let h_z = eta_h(z);
            ((eta * eta - 1.0) * (eta_ab(z) * h_z * h_z + 2.0 * eta_bh(z) * a_z * h_z)
                + (-eta * eta * eta + 3.0 * eta) * a_z * b_z * h_z * h_z)
                * (-cell.q(z)).exp()
                * INV_TWO_PI
        });
        let numeric_bbhh = simpson_integral(cell.left, cell.right, 5000, |z| {
            let eta = cell.eta(z);
            let b_z = eta_b(z);
            let h_z = eta_h(z);
            let bh_z = eta_bh(z);
            (-(2.0 * eta * bh_z * bh_z)
                + (eta * eta - 1.0) * (eta_bb(z) * h_z * h_z + 4.0 * bh_z * b_z * h_z)
                + (-eta * eta * eta + 3.0 * eta) * b_z * b_z * h_z * h_z)
                * (-cell.q(z)).exp()
                * INV_TWO_PI
        });
        let numeric_bhhh = simpson_integral(cell.left, cell.right, 5000, |z| {
            let eta = cell.eta(z);
            let h_z = eta_h(z);
            (-(eta * (3.0 * eta_bh(z) * h_z * h_z))
                + (eta * eta - 1.0) * (3.0 * eta_bh(z) * h_z * h_z)
                + (-eta * eta * eta + 3.0 * eta) * eta_b(z) * h_z * h_z * h_z)
                * (-cell.q(z)).exp()
                * INV_TWO_PI
        });
        let numeric_hhhh = simpson_integral(cell.left, cell.right, 5000, |z| {
            let eta = cell.eta(z);
            let h_z = eta_h(z);
            ((-eta * eta * eta + 3.0 * eta) * h_z * h_z * h_z * h_z)
                * (-cell.q(z)).exp()
                * INV_TWO_PI
        });

        assert!((exact_h - numeric_h).abs() < 1e-8);
        assert!((exact_ah - numeric_ah).abs() < 1e-7);
        assert!((exact_bh - numeric_bh).abs() < 1e-7);
        assert!((exact_hh - numeric_hh).abs() < 1e-7);
        assert!((exact_abh - numeric_abh).abs() < 2e-6);
        assert!((exact_bbh - numeric_bbh).abs() < 2e-6);
        assert!((exact_bhh - numeric_bhh).abs() < 2e-6);
        assert!((exact_hhh - numeric_hhh).abs() < 2e-6);
        assert!((exact_bbbh - numeric_bbbh).abs() < 3e-6);
        assert!((exact_aahh - numeric_aahh).abs() < 3e-6);
        assert!((exact_abhh - numeric_abhh).abs() < 3e-6);
        assert!((exact_bbhh - numeric_bbhh).abs() < 3e-6);
        assert!((exact_bhhh - numeric_bhhh).abs() < 3e-6);
        assert!((exact_hhhh - numeric_hhhh).abs() < 3e-6);
    }

    #[test]
    fn cross_basis_cell_derivatives_match_exact_integrands() {
        let score_span = LocalSpanCubic {
            left: -0.75,
            right: 0.25,
            c0: 0.08,
            c1: -0.03,
            c2: 0.02,
            c3: -0.01,
        };
        let score_basis_span = LocalSpanCubic {
            left: -0.75,
            right: 0.25,
            c0: -0.04,
            c1: 0.06,
            c2: -0.01,
            c3: 0.02,
        };
        let link_span = LocalSpanCubic {
            left: -0.6,
            right: 0.9,
            c0: -0.05,
            c1: 0.04,
            c2: -0.02,
            c3: 0.015,
        };
        let link_basis_span = LocalSpanCubic {
            left: -0.6,
            right: 0.9,
            c0: 0.02,
            c1: -0.01,
            c2: 0.03,
            c3: -0.02,
        };
        let a = 0.3;
        let b = -0.7;
        let coeffs = denested_cell_coefficients(score_span, link_span, a, b);
        let cell = DenestedCubicCell {
            left: score_span.left,
            right: score_span.right,
            c0: coeffs[0],
            c1: coeffs[1],
            c2: coeffs[2],
            c3: coeffs[3],
        };
        let state = evaluate_cell_moments(cell, 24).expect("cell moments");
        let (dc_da, dc_db) = denested_cell_coefficient_partials(score_span, link_span, a, b);
        let (dc_daa, dc_dab, _) = denested_cell_second_partials(score_span, link_span, a, b);

        let coeff_h = score_basis_cell_coefficients(score_basis_span, b);
        let coeff_bh = score_basis_cell_coefficients(score_basis_span, 1.0);
        let coeff_w = link_basis_cell_coefficients(link_basis_span, a, b);
        let (coeff_aw, coeff_bw) = link_basis_cell_coefficient_partials(link_basis_span, a, b);
        let (coeff_aaw, coeff_abw, _) = link_basis_cell_second_partials(link_basis_span, a, b);
        let zero = [0.0; 4];

        let eta_a = |z: f64| 1.0 + link_span.first_derivative(a + b * z);
        let eta_b = |z: f64| z + score_span.evaluate(z) + z * link_span.first_derivative(a + b * z);
        let eta_h = |z: f64| b * score_basis_span.evaluate(z);
        let eta_bh = |z: f64| score_basis_span.evaluate(z);
        let eta_w = |z: f64| link_basis_span.evaluate(a + b * z);
        let eta_ab = |z: f64| z * link_span.second_derivative(a + b * z);
        let eta_aw = |z: f64| link_basis_span.first_derivative(a + b * z);
        let eta_bw = |z: f64| z * link_basis_span.first_derivative(a + b * z);

        let exact_hw =
            cell_second_derivative_from_moments(cell, &coeff_h, &coeff_w, &zero, &state.moments)
                .expect("hw");
        let exact_ahw = cell_third_derivative_from_moments(
            cell,
            &dc_da,
            &coeff_h,
            &coeff_w,
            &zero,
            &coeff_aw,
            &zero,
            &zero,
            &state.moments,
        )
        .expect("ahw");
        let exact_bhw = cell_third_derivative_from_moments(
            cell,
            &dc_db,
            &coeff_h,
            &coeff_w,
            &coeff_bh,
            &coeff_bw,
            &zero,
            &zero,
            &state.moments,
        )
        .expect("bhw");
        let exact_hhw = cell_third_derivative_from_moments(
            cell,
            &coeff_h,
            &coeff_h,
            &coeff_w,
            &zero,
            &zero,
            &zero,
            &zero,
            &state.moments,
        )
        .expect("hhw");
        let exact_hww = cell_third_derivative_from_moments(
            cell,
            &coeff_h,
            &coeff_w,
            &coeff_w,
            &zero,
            &zero,
            &zero,
            &zero,
            &state.moments,
        )
        .expect("hww");
        let exact_aahw = cell_fourth_derivative_from_moments(
            cell,
            &dc_da,
            &dc_da,
            &coeff_h,
            &coeff_w,
            &dc_daa,
            &zero,
            &coeff_aw,
            &zero,
            &coeff_aw,
            &zero,
            &zero,
            &coeff_aaw,
            &zero,
            &zero,
            &zero,
            &state.moments,
        )
        .expect("aahw");
        let exact_hhww = cell_fourth_derivative_from_moments(
            cell,
            &coeff_h,
            &coeff_h,
            &coeff_w,
            &coeff_w,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &state.moments,
        )
        .expect("hhww");
        let exact_hhhw = cell_fourth_derivative_from_moments(
            cell,
            &coeff_h,
            &coeff_h,
            &coeff_h,
            &coeff_w,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &state.moments,
        )
        .expect("hhhw");
        let exact_abhw = cell_fourth_derivative_from_moments(
            cell,
            &dc_da,
            &dc_db,
            &coeff_h,
            &coeff_w,
            &dc_dab,
            &zero,
            &coeff_aw,
            &coeff_bh,
            &coeff_bw,
            &zero,
            &zero,
            &coeff_abw,
            &zero,
            &zero,
            &zero,
            &state.moments,
        )
        .expect("abhw");
        let exact_ahww = cell_fourth_derivative_from_moments(
            cell,
            &dc_da,
            &coeff_h,
            &coeff_w,
            &coeff_w,
            &zero,
            &coeff_aw,
            &coeff_aw,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &state.moments,
        )
        .expect("ahww");
        let exact_bhww = cell_fourth_derivative_from_moments(
            cell,
            &dc_db,
            &coeff_h,
            &coeff_w,
            &coeff_w,
            &coeff_bh,
            &coeff_bw,
            &coeff_bw,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &state.moments,
        )
        .expect("bhww");
        let exact_hwww = cell_fourth_derivative_from_moments(
            cell,
            &coeff_h,
            &coeff_w,
            &coeff_w,
            &coeff_w,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &zero,
            &state.moments,
        )
        .expect("hwww");

        let numeric_hw = simpson_integral(cell.left, cell.right, 5000, |z| {
            (-cell.eta(z) * eta_h(z) * eta_w(z)) * (-cell.q(z)).exp() * INV_TWO_PI
        });
        let numeric_ahw = simpson_integral(cell.left, cell.right, 5000, |z| {
            let eta = cell.eta(z);
            (-(eta * eta_aw(z) * eta_h(z)) + (eta * eta - 1.0) * eta_a(z) * eta_h(z) * eta_w(z))
                * (-cell.q(z)).exp()
                * INV_TWO_PI
        });
        let numeric_bhw = simpson_integral(cell.left, cell.right, 5000, |z| {
            let eta = cell.eta(z);
            (-(eta * (eta_bh(z) * eta_w(z) + eta_bw(z) * eta_h(z)))
                + (eta * eta - 1.0) * eta_b(z) * eta_h(z) * eta_w(z))
                * (-cell.q(z)).exp()
                * INV_TWO_PI
        });
        let numeric_hhw = simpson_integral(cell.left, cell.right, 5000, |z| {
            let eta = cell.eta(z);
            ((eta * eta - 1.0) * eta_h(z) * eta_h(z) * eta_w(z)) * (-cell.q(z)).exp() * INV_TWO_PI
        });
        let numeric_hww = simpson_integral(cell.left, cell.right, 5000, |z| {
            let eta = cell.eta(z);
            ((eta * eta - 1.0) * eta_h(z) * eta_w(z) * eta_w(z)) * (-cell.q(z)).exp() * INV_TWO_PI
        });
        let numeric_aahw = simpson_integral(cell.left, cell.right, 5000, |z| {
            let eta = cell.eta(z);
            (-(eta * polynomial_value(&coeff_aaw, z) * eta_h(z))
                + (eta * eta - 1.0)
                    * (polynomial_value(&dc_daa, z) * eta_h(z) * eta_w(z)
                        + 2.0 * eta_aw(z) * eta_a(z) * eta_h(z))
                + (-eta * eta * eta + 3.0 * eta) * eta_a(z) * eta_a(z) * eta_h(z) * eta_w(z))
                * (-cell.q(z)).exp()
                * INV_TWO_PI
        });
        let numeric_hhww = simpson_integral(cell.left, cell.right, 5000, |z| {
            let eta = cell.eta(z);
            ((-eta * eta * eta + 3.0 * eta) * eta_h(z) * eta_h(z) * eta_w(z) * eta_w(z))
                * (-cell.q(z)).exp()
                * INV_TWO_PI
        });
        let numeric_hhhw = simpson_integral(cell.left, cell.right, 5000, |z| {
            let eta = cell.eta(z);
            ((-eta * eta * eta + 3.0 * eta) * eta_h(z) * eta_h(z) * eta_h(z) * eta_w(z))
                * (-cell.q(z)).exp()
                * INV_TWO_PI
        });
        let numeric_abhw = simpson_integral(cell.left, cell.right, 5000, |z| {
            let eta = cell.eta(z);
            (-(eta * polynomial_value(&coeff_abw, z) * eta_h(z) + eta * eta_aw(z) * eta_bh(z))
                + (eta * eta - 1.0)
                    * (eta_ab(z) * eta_h(z) * eta_w(z)
                        + eta_aw(z) * eta_b(z) * eta_h(z)
                        + eta_bh(z) * eta_a(z) * eta_w(z)
                        + eta_bw(z) * eta_a(z) * eta_h(z))
                + (-eta * eta * eta + 3.0 * eta) * eta_a(z) * eta_b(z) * eta_h(z) * eta_w(z))
                * (-cell.q(z)).exp()
                * INV_TWO_PI
        });
        let numeric_ahww = simpson_integral(cell.left, cell.right, 5000, |z| {
            let eta = cell.eta(z);
            (2.0 * (eta * eta - 1.0) * eta_aw(z) * eta_h(z) * eta_w(z)
                + (-eta * eta * eta + 3.0 * eta) * eta_a(z) * eta_h(z) * eta_w(z) * eta_w(z))
                * (-cell.q(z)).exp()
                * INV_TWO_PI
        });
        let numeric_bhww = simpson_integral(cell.left, cell.right, 5000, |z| {
            let eta = cell.eta(z);
            let h_z = eta_h(z);
            let w_z = eta_w(z);
            ((eta * eta - 1.0) * (eta_bh(z) * w_z * w_z + 2.0 * eta_bw(z) * h_z * w_z)
                + (-eta * eta * eta + 3.0 * eta) * eta_b(z) * h_z * w_z * w_z)
                * (-cell.q(z)).exp()
                * INV_TWO_PI
        });
        let numeric_hwww = simpson_integral(cell.left, cell.right, 5000, |z| {
            let eta = cell.eta(z);
            ((-eta * eta * eta + 3.0 * eta) * eta_h(z) * eta_w(z) * eta_w(z) * eta_w(z))
                * (-cell.q(z)).exp()
                * INV_TWO_PI
        });

        assert!((exact_hw - numeric_hw).abs() < 1e-7);
        assert!((exact_ahw - numeric_ahw).abs() < 2e-6);
        assert!((exact_bhw - numeric_bhw).abs() < 2e-6);
        assert!((exact_hhw - numeric_hhw).abs() < 2e-6);
        assert!((exact_hww - numeric_hww).abs() < 2e-6);
        assert!((exact_aahw - numeric_aahw).abs() < 3e-6);
        assert!((exact_hhww - numeric_hhww).abs() < 3e-6);
        assert!((exact_hhhw - numeric_hhhw).abs() < 3e-6);
        assert!((exact_abhw - numeric_abhw).abs() < 3e-6);
        assert!((exact_ahww - numeric_ahww).abs() < 3e-6);
        assert!((exact_bhww - numeric_bhww).abs() < 3e-6);
        assert!((exact_hwww - numeric_hwww).abs() < 3e-6);
    }

    #[test]
    fn cell_moment_scratch_reuses_buffers_under_margslope_like_pressure() {
        let cells = [
            DenestedCubicCell {
                left: -1.2,
                right: -0.35,
                c0: 0.18,
                c1: 0.72,
                c2: -0.045,
                c3: 0.018,
            },
            DenestedCubicCell {
                left: -0.35,
                right: 0.48,
                c0: -0.08,
                c1: 0.91,
                c2: 0.038,
                c3: -0.014,
            },
            DenestedCubicCell {
                left: 0.48,
                right: 1.4,
                c0: 0.11,
                c1: 0.83,
                c2: 0.022,
                c3: 0.012,
            },
        ];
        let mut scratch = CellMomentScratch::with_capacity(MAX_AFFINE_ANCHOR_DEGREE);
        for cell in cells {
            let baseline = evaluate_cell_moments(cell, 9).expect("baseline moments");
            let scratch_state =
                evaluate_cell_moments_with_scratch(cell, 9, &mut scratch).expect("scratch moments");
            assert_eq!(baseline.branch, scratch_state.branch);
            assert!((baseline.value - scratch_state.value).abs() <= 1e-10);
            assert_eq!(baseline.moments.len(), scratch_state.moments.len());
            for (lhs, rhs) in baseline.moments.iter().zip(scratch_state.moments.iter()) {
                assert!((lhs - rhs).abs() <= 1e-10, "{lhs} vs {rhs}");
            }
        }

        reset_cell_moment_test_reallocs();
        let mut checksum = 0.0;
        for i in 0..5_000 {
            let cell = cells[i % cells.len()];
            let state = evaluate_cell_moments_with_scratch(cell, 9, &mut scratch)
                .expect("scratch moments under repeated pressure");
            checksum += state.value + state.moments[0] * 1e-12;
        }
        assert!(checksum.is_finite());
        assert_eq!(
            cell_moment_test_reallocs(),
            0,
            "scratch-backed inner cell-moment calls should not grow Vec buffers"
        );
    }

    #[test]
    fn evaluate_cell_moments_matches_numeric_integrals() {
        let cell = DenestedCubicCell {
            left: -0.9,
            right: 0.8,
            c0: 0.15,
            c1: -0.35,
            c2: 0.11,
            c3: -0.07,
        };
        let state = evaluate_cell_moments(cell, 6).expect("cell moments");
        let value_numeric = simpson_integral(cell.left, cell.right, 4000, |z| {
            super::normal_cdf(cell.eta(z)) * normal_pdf(z)
        });
        assert!((state.value - value_numeric).abs() < 1e-9);
        for degree in 0..=6 {
            let target = simpson_integral(cell.left, cell.right, 4000, |z| {
                z.powi(degree as i32) * (-cell.q(z)).exp()
            });
            assert!((state.moments[degree] - target).abs() < 1e-9);
        }
    }

    #[test]
    fn partition_builder_moves_link_preimages_with_intercept() {
        let score_breaks = [-2.0, -1.0, 0.0, 1.0, 2.0];
        let link_breaks = [-1.5, -0.5, 0.5, 1.5];
        let score_span = |z: f64| {
            let left = if z < -1.0 {
                -2.0
            } else if z < 0.0 {
                -1.0
            } else if z < 1.0 {
                0.0
            } else {
                1.0
            };
            Ok(LocalSpanCubic {
                left,
                right: left + 1.0,
                c0: 0.1,
                c1: 0.2,
                c2: 0.0,
                c3: 0.0,
            })
        };
        let link_span = |u: f64| {
            let left = if u < -0.5 {
                -1.5
            } else if u < 0.5 {
                -0.5
            } else {
                0.5
            };
            Ok(LocalSpanCubic {
                left,
                right: left + 1.0,
                c0: -0.05,
                c1: 0.1,
                c2: 0.0,
                c3: 0.0,
            })
        };
        let cells_a0 = build_denested_partition_cells(
            0.25,
            0.9,
            &score_breaks,
            &link_breaks,
            score_span,
            link_span,
        )
        .expect("cells a0");
        let cells_a1 = build_denested_partition_cells(
            0.55,
            0.9,
            &score_breaks,
            &link_breaks,
            score_span,
            link_span,
        )
        .expect("cells a1");
        assert!(cells_a0.len() >= score_breaks.len() - 1);
        assert!(
            cells_a0
                .windows(2)
                .all(|w| (w[0].cell.right - w[1].cell.left).abs() <= 1e-12)
        );
        assert!(
            cells_a0
                .iter()
                .zip(cells_a1.iter())
                .any(|(lhs, rhs)| (lhs.cell.left - rhs.cell.left).abs() > 1e-10)
        );
        assert!(cells_a0.first().unwrap().cell.left.is_infinite());
        assert!(cells_a0.last().unwrap().cell.right.is_infinite());
    }

    #[test]
    fn partition_builder_without_breaks_returns_single_global_cell() {
        let cells = build_denested_partition_cells_with_tails(
            0.3,
            -0.4,
            &[],
            &[],
            |z| {
                if z.is_nan() {
                    return Err("probe z is NaN".to_string());
                }
                Ok(LocalSpanCubic {
                    left: 0.0,
                    right: 1.0,
                    c0: 0.0,
                    c1: 0.0,
                    c2: 0.0,
                    c3: 0.0,
                })
            },
            |u| {
                if u.is_nan() {
                    return Err("probe u is NaN".to_string());
                }
                Ok(LocalSpanCubic {
                    left: 0.0,
                    right: 1.0,
                    c0: 0.0,
                    c1: 0.0,
                    c2: 0.0,
                    c3: 0.0,
                })
            },
        )
        .expect("global cell");
        assert_eq!(cells.len(), 1);
        assert_eq!(cells[0].cell.left, f64::NEG_INFINITY);
        assert_eq!(cells[0].cell.right, f64::INFINITY);
        assert!(cells[0].cell.c2.abs() < 1e-12);
        assert!(cells[0].cell.c3.abs() < 1e-12);
    }

    #[test]
    fn polynomial_integral_helper_matches_moment_sum() {
        let cell = DenestedCubicCell {
            left: -1.5,
            right: 1.25,
            c0: 0.2,
            c1: -0.4,
            c2: 0.15,
            c3: 0.03,
        };
        let state = evaluate_cell_moments(cell, 8).expect("cell moments");
        let coeffs = [1.5, -0.25, 0.75, 0.1];
        let expected = INV_TWO_PI
            * coeffs
                .iter()
                .enumerate()
                .map(|(idx, coeff)| coeff * state.moments[idx])
                .sum::<f64>();
        let got = cell_polynomial_integral_from_moments(&coeffs, &state.moments, "test poly")
            .expect("poly integral");
        assert!((got - expected).abs() < 1e-14);
    }

    #[test]
    fn batched_cell_moment_max_degree_matches_direct_non_affine_grid() {
        let cells = [
            DenestedCubicCell {
                left: -2.0,
                right: -0.25,
                c0: -0.7,
                c1: 0.8,
                c2: 0.015,
                c3: -0.004,
            },
            DenestedCubicCell {
                left: -0.5,
                right: 0.75,
                c0: 0.2,
                c1: -0.35,
                c2: -0.025,
                c3: 0.0,
            },
            DenestedCubicCell {
                left: 0.1,
                right: 1.6,
                c0: 0.4,
                c1: 0.25,
                c2: 0.01,
                c3: 0.006,
            },
            DenestedCubicCell {
                left: -1.25,
                right: 2.25,
                c0: -0.1,
                c1: 0.55,
                c2: -0.012,
                c3: 0.003,
            },
        ];
        for cell in cells {
            let branch = branch_cell(cell).expect("branch");
            if branch == ExactCellBranch::Affine {
                continue;
            }
            let batched =
                evaluate_non_affine_cell_state(cell, branch, 21).expect("degree-21 state");
            for degree in [9usize, 15, 21] {
                let direct =
                    evaluate_non_affine_cell_state(cell, branch, degree).expect("direct state");
                assert_eq!(batched.branch, direct.branch);
                let denom = direct.value.abs().max(1.0);
                assert!(((batched.value - direct.value).abs() / denom) < 1e-10);
                for k in 0..=degree {
                    let denom = direct.moments[k].abs().max(1.0);
                    let rel = (batched.moments[k] - direct.moments[k]).abs() / denom;
                    assert!(
                        rel < 1e-10,
                        "cell={cell:?} degree={degree} moment={k} rel={rel:e}"
                    );
                }
            }
        }
    }

    #[test]
    fn derivative_moment_evaluator_matches_value_evaluator_moments() {
        let cells = [
            DenestedCubicCell {
                left: -2.0,
                right: -0.4,
                c0: 0.15,
                c1: -0.8,
                c2: 0.0,
                c3: 0.0,
            },
            DenestedCubicCell {
                left: -0.75,
                right: 1.4,
                c0: -0.25,
                c1: 0.6,
                c2: 0.12,
                c3: 0.0,
            },
            DenestedCubicCell {
                left: -1.1,
                right: 0.9,
                c0: 0.35,
                c1: -0.3,
                c2: 0.05,
                c3: -0.015,
            },
        ];
        for cell in cells {
            for degree in [4usize, 9, 15, 21] {
                let full = evaluate_cell_moments_uncached(cell, degree).expect("full moments");
                let derivative = evaluate_cell_derivative_moments_uncached(cell, degree)
                    .expect("derivative moments");
                assert_eq!(full.branch, derivative.branch);
                assert_eq!(full.moments.len(), derivative.moments.len());
                for k in 0..full.moments.len() {
                    assert_eq!(full.moments[k].to_bits(), derivative.moments[k].to_bits());
                }
            }
        }
    }

    #[test]
    fn cell_moment_lru_matches_uncached_non_affine_grid() {
        let cache = CellMomentLruCache::new(16 * 1024 * 1024);
        let stats = CellMomentCacheStats::default();
        let c0s = [-0.75, 0.0, 0.5];
        let c1s = [-1.2, 0.25, 1.1];
        let c2s = [-0.18, 0.07];
        let c3s = [0.0, 0.025];
        let bounds = [(-2.0, -0.5), (-0.25, 1.5)];
        let degrees = [4usize, 9, 15, 21];
        for &c0 in &c0s {
            for &c1 in &c1s {
                for &c2 in &c2s {
                    for &c3 in &c3s {
                        for &(left, right) in &bounds {
                            for &max_degree in &degrees {
                                let cell = DenestedCubicCell {
                                    left,
                                    right,
                                    c0,
                                    c1,
                                    c2,
                                    c3,
                                };
                                let branch = branch_cell(cell).expect("branch");
                                if branch == ExactCellBranch::Affine {
                                    continue;
                                }
                                let expected =
                                    evaluate_non_affine_cell_state(cell, branch, max_degree)
                                        .expect("uncached non-affine moments");
                                let got = evaluate_cell_moments_cached(
                                    cell,
                                    max_degree,
                                    &cache,
                                    Some(&stats),
                                )
                                .expect("cached moments");
                                assert_eq!(got.branch, expected.branch);
                                assert_eq!(got.moments.len(), max_degree + 1);
                                let denom = expected.value.abs().max(1.0);
                                assert!(
                                    ((got.value - expected.value).abs() / denom) < 1e-10,
                                    "value mismatch for {cell:?} degree {max_degree}: got {} expected {}",
                                    got.value,
                                    expected.value
                                );
                                for (idx, (&lhs, &rhs)) in
                                    got.moments.iter().zip(expected.moments.iter()).enumerate()
                                {
                                    let denom = rhs.abs().max(1.0);
                                    assert!(
                                        ((lhs - rhs).abs() / denom) < 1e-10,
                                        "moment {idx} mismatch for {cell:?} degree {max_degree}: got {lhs} expected {rhs}"
                                    );
                                }
                                let warm = evaluate_cell_moments_cached(
                                    cell,
                                    max_degree,
                                    &cache,
                                    Some(&stats),
                                )
                                .expect("warm cached moments");
                                assert_eq!(warm, got);
                            }
                        }
                    }
                }
            }
        }
        let (hits, misses) = stats.snapshot();
        assert!(hits > 0, "expected warm LRU hits");
        assert!(misses > 0, "expected cold LRU misses");
    }

    #[test]
    fn cell_moment_fingerprint_exact_cache_matches_current_evaluator() {
        let cells = [
            DenestedCubicCell {
                left: -1.75,
                right: -0.25,
                c0: 0.15,
                c1: -0.35,
                c2: 0.08,
                c3: -0.015,
            },
            DenestedCubicCell {
                left: -0.5,
                right: 0.8,
                c0: -0.2,
                c1: 0.45,
                c2: -0.12,
                c3: 0.025,
            },
            DenestedCubicCell {
                left: 0.1,
                right: 1.6,
                c0: 0.05,
                c1: 0.2,
                c2: 0.03,
                c3: 0.004,
            },
        ];
        let mut cache = std::collections::HashMap::new();
        for max_degree in [0usize, 3, 4, 9, 16] {
            for cell in cells {
                let baseline = evaluate_cell_moments(cell, max_degree).expect("baseline moments");
                let key = cell_moment_cache_key(cell, max_degree, 0.0);
                let cached = cache.entry(key).or_insert_with(|| {
                    evaluate_cell_moments(cell, max_degree).expect("cached moments")
                });
                assert_eq!(baseline.branch, cached.branch);
                assert_eq!(baseline.value.to_bits(), cached.value.to_bits());
                assert_eq!(baseline.moments.len(), cached.moments.len());
                for (lhs, rhs) in baseline.moments.iter().zip(cached.moments.iter()) {
                    assert_eq!(lhs.to_bits(), rhs.to_bits());
                }
            }
        }
    }

    #[test]
    fn fuzzy_cell_moment_fingerprint_error_scales_with_epsilon() {
        for epsilon in [1e-8, 1e-6] {
            let base = DenestedCubicCell {
                left: -1.25,
                right: 1.1,
                c0: 0.1,
                c1: -0.25,
                c2: 0.04,
                c3: -0.006,
            };
            let perturbed = DenestedCubicCell {
                left: base.left + 0.001 * epsilon,
                right: base.right - 0.001 * epsilon,
                c0: base.c0 + 0.001 * epsilon,
                c1: base.c1 - 0.001 * epsilon,
                c2: base.c2 + 0.001 * epsilon,
                c3: base.c3 - 0.001 * epsilon,
            };
            assert_eq!(
                cell_moment_cache_key(base, 9, epsilon),
                cell_moment_cache_key(perturbed, 9, epsilon)
            );
            let lhs = evaluate_cell_moments(base, 9).expect("base moments");
            let rhs = evaluate_cell_moments(perturbed, 9).expect("perturbed moments");
            let max_rel = lhs
                .moments
                .iter()
                .zip(rhs.moments.iter())
                .map(|(a, b)| (a - b).abs() / a.abs().max(b.abs()).max(1.0))
                .fold(0.0_f64, f64::max);
            assert!(
                max_rel <= 10.0 * epsilon,
                "epsilon={epsilon:.1e} max_rel={max_rel:.3e}"
            );
        }
    }

    /// Locks in numerical equivalence of the optimized
    /// `evaluate_non_affine_cell_state` against an inline reference
    /// implementation that mirrors the prior pre-fold structure
    /// (separate `cell.eta(z)` / `cell.q(z)` calls; post-loop
    /// `* half_width`; trailing `value_integral * half_width / sqrt(TAU)`).
    /// Any drift larger than 1e-13 relative would indicate the hot-path
    /// rewrite changed the math.
    #[test]
    fn non_affine_cell_state_matches_prefold_reference_to_1e_minus_13() {
        // Reference: byte-for-byte the structure of the previous
        // implementation. Kept local to this test to avoid leaking a second
        // public surface.
        fn reference(
            cell: DenestedCubicCell,
            branch: ExactCellBranch,
            max_degree: usize,
        ) -> CellMomentState {
            let mut moments: CellMomentVec = smallvec![0.0_f64; max_degree + 1];
            let mut value_integral = 0.0_f64;
            let center = 0.5 * (cell.left + cell.right);
            let half_width = 0.5 * (cell.right - cell.left);
            for (&node, &weight) in GL_NODES.iter().zip(GL_WEIGHTS.iter()) {
                let z = center + half_width * node;
                let eta = cell.eta(z);
                let moment_weight = weight * (-cell.q(z)).exp();
                let mut z_pow = 1.0_f64;
                for moment in &mut moments {
                    *moment = moment_weight.mul_add(z_pow, *moment);
                    z_pow *= z;
                }
                value_integral += weight * (-0.5 * z * z).exp() * normal_cdf(eta);
            }
            for moment in &mut moments {
                *moment *= half_width;
            }
            CellMomentState {
                branch,
                value: value_integral * half_width / (std::f64::consts::TAU).sqrt(),
                moments,
            }
        }

        // Hand-rolled inputs that cross both Quartic and Sextic branches and
        // exercise positive/negative coefficients, asymmetric intervals, and
        // a wide degree range (matches survival_marginal_slope's degree=9
        // production call as well as the bernoulli outer-step degree=24).
        let cells = [
            DenestedCubicCell {
                left: -1.25,
                right: -0.2,
                c0: -0.35,
                c1: 0.85,
                c2: 0.04,
                c3: -0.015,
            },
            DenestedCubicCell {
                left: -0.2,
                right: 0.55,
                c0: 0.12,
                c1: -0.65,
                c2: -0.025,
                c3: 0.02,
            },
            DenestedCubicCell {
                left: 0.55,
                right: 1.6,
                c0: 0.42,
                c1: 0.35,
                c2: 0.018,
                c3: 0.012,
            },
            DenestedCubicCell {
                left: -3.0,
                right: -1.0,
                c0: 1.7,
                c1: -0.4,
                c2: 0.11,
                c3: -0.07,
            },
        ];
        let degrees = [0_usize, 4, 9, 16, 24];
        for cell in cells {
            let branch = branch_cell(cell).expect("branch");
            assert_ne!(branch, ExactCellBranch::Affine);
            for max_degree in degrees {
                let actual = evaluate_non_affine_cell_state(cell, branch, max_degree)
                    .expect("optimized non-affine");
                let expected = reference(cell, branch, max_degree);
                assert_eq!(actual.branch, expected.branch);
                assert_eq!(actual.moments.len(), expected.moments.len());
                let denom_v = expected.value.abs().max(1.0);
                let rel_v = (actual.value - expected.value).abs() / denom_v;
                let actual_v = actual.value;
                let expected_v = expected.value;
                assert!(
                    rel_v <= 1e-13,
                    "value rel mismatch for {cell:?} degree {max_degree}: \
                     actual={actual_v:.17e} expected={expected_v:.17e} rel={rel_v:.3e}"
                );
                for (k, (lhs, rhs)) in actual
                    .moments
                    .iter()
                    .zip(expected.moments.iter())
                    .enumerate()
                {
                    let denom = rhs.abs().max(1.0);
                    let rel = (lhs - rhs).abs() / denom;
                    assert!(
                        rel <= 1e-13,
                        "moment {k} rel mismatch for {cell:?} degree {max_degree}: \
                         actual={lhs:.17e} expected={rhs:.17e} rel={rel:.3e}"
                    );
                }

                // Also lock in the derivative-state path on the same
                // inputs so the (parallel) edit there can't drift.
                let actual_deriv =
                    evaluate_non_affine_cell_derivative_state(cell, branch, max_degree)
                        .expect("optimized derivative");
                for (k, (lhs, rhs)) in actual_deriv
                    .moments
                    .iter()
                    .zip(expected.moments.iter())
                    .enumerate()
                {
                    let denom = rhs.abs().max(1.0);
                    let rel = (lhs - rhs).abs() / denom;
                    assert!(
                        rel <= 1e-13,
                        "deriv moment {k} rel mismatch for {cell:?} degree {max_degree}: \
                         actual={lhs:.17e} expected={rhs:.17e} rel={rel:.3e}"
                    );
                }
            }
        }
    }

    /// DECISIVE: the third-derivative kernel must equal the FD of the
    /// second-derivative kernel w.r.t. a parameter that perturbs `eta`,
    /// RE-EVALUATING the moments at each step (the moments depend on `eta`
    /// via the `exp(-q)` weight). This isolates the kernel from all survival
    /// partition/cross machinery (gam#979 f_uv_dir localization).
    #[test]
    fn third_derivative_kernel_matches_fd_of_second_with_eta_perturbation() {
        // A finite, non-affine cell.
        let base = DenestedCubicCell {
            left: -0.6,
            right: 0.9,
            c0: 0.30,
            c1: 0.45,
            c2: -0.20,
            c3: 0.12,
        };
        // Synthetic parameter directions as cubic-in-z perturbations of eta:
        //   eta_u = ∂eta/∂u, eta_v = ∂eta/∂v, eta_t = ∂eta/∂t (the dir).
        let eta_u = [0.11_f64, -0.07, 0.05, 0.02];
        let eta_v = [-0.09_f64, 0.13, -0.04, 0.03];
        let eta_t = [0.17_f64, 0.06, -0.10, 0.04]; // the "b-like" direction
        // Second crosses ∂²eta/∂{·}{·} (pick small non-zero cubics).
        let eta_uv = [0.02_f64, 0.01, -0.015, 0.005];
        let eta_ut = [-0.01_f64, 0.02, 0.007, -0.003];
        let eta_vt = [0.015_f64, -0.008, 0.01, 0.004];
        // Third cross ∂³eta/∂u∂v∂t.
        let eta_uvt = [0.003_f64, -0.002, 0.001, 0.0005];

        let neg = |a: &[f64; 4]| a.map(|v| -v);
        let max_degree = 15usize;

        // f_uv(s) where param s shifts eta by s·(eta_t + ½ s²... ) — here we
        // build the cell at eta + s·eta_t + s²·eta_vt-style is NOT needed; we
        // only need the t-direction to first order for ∂/∂t. To FD ∂(f_uv)/∂t
        // we perturb eta along eta_t AND carry the s-dependence of the u,v
        // crosses: eta_u(s)=eta_u + s·eta_ut, eta_v(s)=eta_v + s·eta_vt,
        // eta_uv(s)=eta_uv + s·eta_uvt. The cell cubic shifts by s·eta_t.
        let f_uv_at = |s: f64| -> f64 {
            let cell_s = DenestedCubicCell {
                c0: base.c0 + s * eta_t[0],
                c1: base.c1 + s * eta_t[1],
                c2: base.c2 + s * eta_t[2],
                c3: base.c3 + s * eta_t[3],
                ..base
            };
            // Moments MUST be recomputed at the perturbed eta.
            let st = evaluate_cell_moments(cell_s, max_degree).unwrap();
            let neg_cell = DenestedCubicCell {
                c0: -cell_s.c0,
                c1: -cell_s.c1,
                c2: -cell_s.c2,
                c3: -cell_s.c3,
                ..cell_s
            };
            let u_s = [
                eta_u[0] + s * eta_ut[0],
                eta_u[1] + s * eta_ut[1],
                eta_u[2] + s * eta_ut[2],
                eta_u[3] + s * eta_ut[3],
            ];
            let v_s = [
                eta_v[0] + s * eta_vt[0],
                eta_v[1] + s * eta_vt[1],
                eta_v[2] + s * eta_vt[2],
                eta_v[3] + s * eta_vt[3],
            ];
            let uv_s = [
                eta_uv[0] + s * eta_uvt[0],
                eta_uv[1] + s * eta_uvt[1],
                eta_uv[2] + s * eta_uvt[2],
                eta_uv[3] + s * eta_uvt[3],
            ];
            cell_second_derivative_from_moments(
                neg_cell,
                &neg(&u_s),
                &neg(&v_s),
                &neg(&uv_s),
                &st.moments,
            )
            .unwrap()
        };

        let h = 1e-5;
        let fd = (f_uv_at(h) - f_uv_at(-h)) / (2.0 * h);

        // Analytic third via the kernel (negated cell + negated crosses, as the
        // survival path does).
        let st0 = evaluate_cell_moments(base, max_degree).unwrap();
        let neg_cell0 = DenestedCubicCell {
            c0: -base.c0,
            c1: -base.c1,
            c2: -base.c2,
            c3: -base.c3,
            ..base
        };
        let analytic = cell_third_derivative_from_moments(
            neg_cell0,
            &neg(&eta_u),
            &neg(&eta_v),
            &neg(&eta_t),
            &neg(&eta_uv),
            &neg(&eta_ut),
            &neg(&eta_vt),
            &neg(&eta_uvt),
            &st0.moments,
        )
        .unwrap();

        let denom = fd.abs().max(1e-3);
        let rel = (analytic - fd).abs() / denom;
        assert!(
            rel <= 1e-5,
            "third kernel vs FD-of-second mismatch: analytic={analytic:.12e} fd={fd:.12e} rel={rel:.3e}"
        );
    }

    #[test]
    fn moving_shared_edge_second_integral_derivative_has_leibniz_jump_sign() {
        let edge0 = 0.2_f64;
        let edge_velocity = -0.37_f64;

        let left_eta = [0.22_f64, -0.18, 0.09, 0.03];
        let right_eta = [-0.11_f64, 0.26, -0.04, 0.02];
        let left_r = [0.08_f64, -0.05, 0.03, 0.01];
        let left_s = [-0.06_f64, 0.04, 0.02, -0.015];
        let left_rs = [0.025_f64, -0.012, 0.006, 0.004];
        let right_r = [-0.03_f64, 0.07, -0.02, 0.012];
        let right_s = [0.05_f64, -0.025, 0.018, 0.007];
        let right_rs = [-0.018_f64, 0.014, -0.005, 0.003];

        let integral_at = |shift: f64| -> f64 {
            let edge = edge0 + edge_velocity * shift;
            let left = DenestedCubicCell {
                left: -0.7,
                right: edge,
                c0: left_eta[0],
                c1: left_eta[1],
                c2: left_eta[2],
                c3: left_eta[3],
            };
            let right = DenestedCubicCell {
                left: edge,
                right: 1.1,
                c0: right_eta[0],
                c1: right_eta[1],
                c2: right_eta[2],
                c3: right_eta[3],
            };
            let left_state = evaluate_cell_moments(left, 12).expect("left moments");
            let right_state = evaluate_cell_moments(right, 12).expect("right moments");
            cell_second_derivative_from_moments(
                left,
                &left_r,
                &left_s,
                &left_rs,
                &left_state.moments,
            )
            .expect("left second")
                + cell_second_derivative_from_moments(
                    right,
                    &right_r,
                    &right_s,
                    &right_rs,
                    &right_state.moments,
                )
                .expect("right second")
        };

        let h = 1e-5;
        let fd = (integral_at(h) - integral_at(-h)) / (2.0 * h);

        let left = DenestedCubicCell {
            left: -0.7,
            right: edge0,
            c0: left_eta[0],
            c1: left_eta[1],
            c2: left_eta[2],
            c3: left_eta[3],
        };
        let right = DenestedCubicCell {
            left: edge0,
            right: 1.1,
            c0: right_eta[0],
            c1: right_eta[1],
            c2: right_eta[2],
            c3: right_eta[3],
        };
        let f_left =
            cell_second_derivative_boundary_integrand(left, &left_r, &left_s, &left_rs, edge0);
        let f_right =
            cell_second_derivative_boundary_integrand(right, &right_r, &right_s, &right_rs, edge0);
        let analytic = edge_velocity * (f_left - f_right);

        let denom = analytic.abs().max(1e-8);
        let rel = (fd - analytic).abs() / denom;
        assert!(
            rel <= 5e-8,
            "moving edge sign mismatch: fd={fd:.12e} analytic={analytic:.12e} rel={rel:.3e}"
        );
    }

    #[test]
    fn moving_shared_edge_second_integral_mixed_derivative_has_full_leibniz_terms() {
        let edge0 = -0.15_f64;
        let edge_d1 = 0.31_f64;
        let edge_d2 = -0.27_f64;
        let edge_d12 = 0.19_f64;

        let left_eta = [0.16_f64, -0.21, 0.07, -0.025];
        let right_eta = [-0.09_f64, 0.18, -0.055, 0.018];
        let left_r = [0.075_f64, -0.045, 0.018, 0.009];
        let left_s = [-0.052_f64, 0.033, 0.014, -0.011];
        let left_rs = [0.021_f64, -0.009, 0.005, 0.0025];
        let right_r = [-0.028_f64, 0.063, -0.017, 0.010];
        let right_s = [0.047_f64, -0.023, 0.016, 0.006];
        let right_rs = [-0.015_f64, 0.012, -0.004, 0.002];

        let integral_at = |s1: f64, s2: f64| -> f64 {
            let edge = edge0 + edge_d1 * s1 + edge_d2 * s2 + edge_d12 * s1 * s2;
            let left = DenestedCubicCell {
                left: -0.8,
                right: edge,
                c0: left_eta[0],
                c1: left_eta[1],
                c2: left_eta[2],
                c3: left_eta[3],
            };
            let right = DenestedCubicCell {
                left: edge,
                right: 0.9,
                c0: right_eta[0],
                c1: right_eta[1],
                c2: right_eta[2],
                c3: right_eta[3],
            };
            let left_state = evaluate_cell_moments(left, 12).expect("left moments");
            let right_state = evaluate_cell_moments(right, 12).expect("right moments");
            cell_second_derivative_from_moments(
                left,
                &left_r,
                &left_s,
                &left_rs,
                &left_state.moments,
            )
            .expect("left second")
                + cell_second_derivative_from_moments(
                    right,
                    &right_r,
                    &right_s,
                    &right_rs,
                    &right_state.moments,
                )
                .expect("right second")
        };

        let h = 2e-4;
        let fd = (integral_at(h, h) - integral_at(h, -h) - integral_at(-h, h)
            + integral_at(-h, -h))
            / (4.0 * h * h);

        let left = DenestedCubicCell {
            left: -0.8,
            right: edge0,
            c0: left_eta[0],
            c1: left_eta[1],
            c2: left_eta[2],
            c3: left_eta[3],
        };
        let right = DenestedCubicCell {
            left: edge0,
            right: 0.9,
            c0: right_eta[0],
            c1: right_eta[1],
            c2: right_eta[2],
            c3: right_eta[3],
        };

        let boundary_z_derivative =
            |cell: DenestedCubicCell, r: &[f64], s: &[f64], rs: &[f64]| -> f64 {
                let eta = cell.eta(edge0);
                let eta_z = cell.c1 + 2.0 * cell.c2 * edge0 + 3.0 * cell.c3 * edge0 * edge0;
                let cr = poly_eval_at(r, edge0);
                let cs = poly_eval_at(s, edge0);
                let crs = poly_eval_at(rs, edge0);
                let cr_z = r.iter().enumerate().skip(1).fold(0.0, |acc, (k, val)| {
                    acc + (k as f64) * val * edge0.powi(k as i32 - 1)
                });
                let cs_z = s.iter().enumerate().skip(1).fold(0.0, |acc, (k, val)| {
                    acc + (k as f64) * val * edge0.powi(k as i32 - 1)
                });
                let crs_z = rs.iter().enumerate().skip(1).fold(0.0, |acc, (k, val)| {
                    acc + (k as f64) * val * edge0.powi(k as i32 - 1)
                });
                let amp = crs - eta * cr * cs;
                let amp_z = crs_z - eta_z * cr * cs - eta * cr_z * cs - eta * cr * cs_z;
                let q_z = edge0 + eta * eta_z;
                (amp_z - amp * q_z) * (-cell.q(edge0)).exp() * INV_TWO_PI
            };

        let f_left =
            cell_second_derivative_boundary_integrand(left, &left_r, &left_s, &left_rs, edge0);
        let f_right =
            cell_second_derivative_boundary_integrand(right, &right_r, &right_s, &right_rs, edge0);
        let fz_left = boundary_z_derivative(left, &left_r, &left_s, &left_rs);
        let fz_right = boundary_z_derivative(right, &right_r, &right_s, &right_rs);
        let analytic = edge_d12 * (f_left - f_right) + edge_d1 * edge_d2 * (fz_left - fz_right);

        let denom = analytic.abs().max(1e-8);
        let rel = (fd - analytic).abs() / denom;
        assert!(
            rel <= 2e-7,
            "moving edge mixed term mismatch: fd={fd:.12e} analytic={analytic:.12e} rel={rel:.3e}"
        );
    }

    // gam#1454 resolution. The reported defect ("survival flex directional
    // third[g,w0] wrong: candidate f_au_dir/f_aa_dir missing self-flux") posited
    // a MISSING third-order Leibniz self-flux at the moving link-knot crossings.
    // This regression establishes the two facts that, together, prove the
    // implicit-intercept third-order tower
    // (`row_primary_third_contracted_recompute*`) is CORRECT to add no such flux:
    //
    //   (1) The third-derivative integrand `F_rst` genuinely DOES jump across a
    //       C²-link knot — its third coefficient slice carries `c_rst ∝ 6·α₃`,
    //       and `α₃` (the spline's third `z`-derivative) is the one piece a C²
    //       cubic spline leaves discontinuous. So the jump is real and the
    //       `cell_third_derivative_boundary_integrand` flux formula is exact
    //       (verified by FD of a direct ∂/∂edge of the third-integral sum —
    //       a FOURTH-order scenario that pins the integrand, not the tower).
    //
    //   (2) Every boundary term in the Leibniz expansion of a THIRD derivative,
    //       however, evaluates an integrand of order ≤ 2 at the moving edge
    //       (one of the three differentiations is spent moving the boundary).
    //       The second-derivative integrand `F_rs` is CONTINUOUS across the same
    //       C² knot (its slices reach at most `α₂ + 3α₃·shift`, i.e. ½·η''(u*),
    //       which a C² spline keeps continuous). Hence the shared-edge flux
    //       `velocity·(F_rs^L − F_rs^R)` telescopes to ZERO, and the tower's
    //       third-order self-flux is a genuine no-op. The real residual lives in
    //       the interior implicit-intercept assembly, not at the boundary.
    #[test]
    fn third_order_self_flux_telescopes_but_third_integrand_jumps_at_c2_knot_1454() {
        let edge0 = 0.13_f64;
        let edge_velocity = -0.41_f64;

        // Build η continuous to C² at edge0 but with a jump in the cubic (3rd
        // derivative) coefficient. Pick the left cubic freely; choose the right
        // cubic to match value+1st+2nd derivative at edge0, then perturb its c3.
        let left_eta = [0.18_f64, -0.12, 0.07, 0.04];
        let right_c3 = 0.04_f64 + 0.09; // α₃ jump across the knot.
        // Match η, η', η'' at edge0 for the right piece given its c3:
        //   η(z)  = c0 + c1 z + c2 z² + c3 z³
        //   η'(z) = c1 + 2 c2 z + 3 c3 z²
        //   η''(z)= 2 c2 + 6 c3 z
        // Solve right (c0,c1,c2) so the three values equal the left ones at edge0.
        let l0 = left_eta[0];
        let l1 = left_eta[1];
        let l2 = left_eta[2];
        let l3 = left_eta[3];
        let e = edge0;
        let eta_val = l0 + l1 * e + l2 * e * e + l3 * e * e * e;
        let eta_d1 = l1 + 2.0 * l2 * e + 3.0 * l3 * e * e;
        let eta_d2 = 2.0 * l2 + 6.0 * l3 * e;
        let rc2 = (eta_d2 - 6.0 * right_c3 * e) / 2.0;
        let rc1 = eta_d1 - 2.0 * rc2 * e - 3.0 * right_c3 * e * e;
        let rc0 = eta_val - rc1 * e - rc2 * e * e - right_c3 * e * e * e;
        let right_eta = [rc0, rc1, rc2, right_c3];

        // Coefficient slices. The first/second slices we keep continuous at the
        // edge (mimicking c_r=1+η', c_rs∝η'' which a C² spline matches), so the
        // 2nd-order flux would cancel. The third-order slice `rst` carries the
        // jumping α₃ and is DIFFERENT across the edge — this is the term that
        // breaks cancellation.
        let common_r = [0.06_f64, -0.04, 0.02, 0.0];
        let common_s = [-0.05_f64, 0.03, 0.015, 0.0];
        let common_t = [0.08_f64, 0.05, -0.03, 0.0];
        let common_rs = [0.02_f64, -0.01, 0.005, 0.0];
        let common_rt = [-0.012_f64, 0.008, 0.004, 0.0];
        let common_st = [0.015_f64, -0.006, 0.003, 0.0];
        // rst ∝ 6·α₃ in the real path: left and right differ by the α₃ jump.
        let left_rst = [6.0 * l3, 0.0, 0.0, 0.0];
        let right_rst = [6.0 * right_c3, 0.0, 0.0, 0.0];

        let max_degree = 15usize;
        let neg = |a: &[f64; 4]| a.map(|v| -v);

        // The integral sum over the two cells sharing the moving edge, computed
        // via the fixed-domain moment reduction with the SURVIVAL/probit sign
        // convention (negated cell + negated coefficient slices), exactly as the
        // production `row_primary_third_contracted_recompute` path does.
        let integral_at = |shift: f64| -> f64 {
            let edge = edge0 + edge_velocity * shift;
            let left = DenestedCubicCell {
                left: -0.7,
                right: edge,
                c0: left_eta[0],
                c1: left_eta[1],
                c2: left_eta[2],
                c3: left_eta[3],
            };
            let right = DenestedCubicCell {
                left: edge,
                right: 1.0,
                c0: right_eta[0],
                c1: right_eta[1],
                c2: right_eta[2],
                c3: right_eta[3],
            };
            let lst = evaluate_cell_moments(left, max_degree).unwrap();
            let rst_m = evaluate_cell_moments(right, max_degree).unwrap();
            let neg_left = DenestedCubicCell {
                c0: -left.c0,
                c1: -left.c1,
                c2: -left.c2,
                c3: -left.c3,
                ..left
            };
            let neg_right = DenestedCubicCell {
                c0: -right.c0,
                c1: -right.c1,
                c2: -right.c2,
                c3: -right.c3,
                ..right
            };
            let li = cell_third_derivative_from_moments(
                neg_left,
                &neg(&common_r),
                &neg(&common_s),
                &neg(&common_t),
                &neg(&common_rs),
                &neg(&common_rt),
                &neg(&common_st),
                &neg(&left_rst),
                &lst.moments,
            )
            .unwrap();
            let ri = cell_third_derivative_from_moments(
                neg_right,
                &neg(&common_r),
                &neg(&common_s),
                &neg(&common_t),
                &neg(&common_rs),
                &neg(&common_rt),
                &neg(&common_st),
                &neg(&right_rst),
                &rst_m.moments,
            )
            .unwrap();
            li + ri
        };

        let h = 1e-5;
        let fd = (integral_at(h) - integral_at(-h)) / (2.0 * h);

        // Fixed-domain part: differentiate ONLY the integrands (domain frozen at
        // edge0). Its directional derivative is the analytic Leibniz flux alone,
        // since the integrand coefficients here are edge-independent:
        //   flux = velocity · ( F_rst^L(edge0) − F_rst^R(edge0) ).
        //
        // CONVENTION: the finite-difference `integral_at` above integrates the
        // SURVIVAL/probit sign convention — negated cell (η→−η) AND negated
        // coefficient slices — exactly as the production
        // `row_primary_third_contracted_recompute` path does. The Leibniz
        // boundary integrand must therefore be evaluated in that SAME negated
        // convention: the third-derivative integrand is ODD under the joint
        // (η→−η, coeff→−coeff) negation (its `rst`, `η·rs·t`, and `(η²−1)·r·s·t`
        // terms each flip sign an odd number of times), so evaluating the flux
        // with un-negated cells/coeffs yields exactly the opposite sign and the
        // Leibniz identity `fd = flux` fails as `fd = −flux`. (The
        // second-derivative sibling test `moving_shared_edge_second_integral_
        // derivative_has_leibniz_jump_sign` keeps BOTH sides un-negated and so
        // stays self-consistent; this test keeps BOTH sides negated.)
        let neg_eta = |eta: &[f64; 4]| [-eta[0], -eta[1], -eta[2], -eta[3]];
        let left_eta_neg = neg_eta(&left_eta);
        let right_eta_neg = neg_eta(&right_eta);
        let left0 = DenestedCubicCell {
            left: -0.7,
            right: edge0,
            c0: left_eta_neg[0],
            c1: left_eta_neg[1],
            c2: left_eta_neg[2],
            c3: left_eta_neg[3],
        };
        let right0 = DenestedCubicCell {
            left: edge0,
            right: 1.0,
            c0: right_eta_neg[0],
            c1: right_eta_neg[1],
            c2: right_eta_neg[2],
            c3: right_eta_neg[3],
        };
        let f_left = cell_third_derivative_boundary_integrand(
            left0,
            &neg(&common_r),
            &neg(&common_s),
            &neg(&common_t),
            &neg(&common_rs),
            &neg(&common_rt),
            &neg(&common_st),
            &neg(&left_rst),
            edge0,
        );
        let f_right = cell_third_derivative_boundary_integrand(
            right0,
            &neg(&common_r),
            &neg(&common_s),
            &neg(&common_t),
            &neg(&common_rs),
            &neg(&common_rt),
            &neg(&common_st),
            &neg(&right_rst),
            edge0,
        );

        // The integrand DOES jump across this C² knot (the α₃ third-coefficient
        // term is the only discontinuous piece). Confirm the jump is genuine —
        // if it were zero the flux would be a no-op and #1454 would not exist.
        let jump = f_left - f_right;
        assert!(
            jump.abs() > 1e-4,
            "third-derivative integrand must jump across the C² knot (α₃ discontinuity); \
             got jump={jump:.3e}"
        );

        let analytic_flux = edge_velocity * jump;
        let denom = fd.abs().max(1e-6);
        let rel = (fd - analytic_flux).abs() / denom;
        assert!(
            rel <= 1e-5,
            "moving-edge third-derivative flux mismatch (#1454): fd={fd:.12e} \
             analytic_flux={analytic_flux:.12e} rel={rel:.3e}"
        );

        // ---- Fact (2): the SECOND-derivative integrand telescopes to zero. ----
        // A 3rd-derivative Leibniz boundary term spends one differentiation on
        // the moving edge and evaluates a ≤2nd-order integrand there. The
        // hardest such term is the slope-slope Hessian integrand `F_bb`, whose
        // coefficient slice is the link cubic's b-b partial
        //   dc_dbb(z) = [0, 0, 2(α₂ + 3 α₃·shift), 6 α₃·b]·(z⁰..z³)
        //             = z²·η''(u),  with u = a + b·z, shift = a − knot.
        // Across a C² knot α₂, α₃, and `shift` all jump, yet η''(u*) is
        // continuous — so the EVALUATED slice `c_bb(z*) = z*²·η''(u*)` matches on
        // both sides and `F_bb` is continuous. Build the two pieces' raw dc_dbb
        // decompositions from `link_cubic_second_partials` and confirm the
        // second-derivative integrand carries no jump (flux telescopes to 0).
        let a_row = 0.21_f64;
        let b_row = 1.37_f64;
        let knot = a_row + b_row * edge0; // u-location of the crossing.
        // Left/right link pieces: choose α₂,α₃ freely on the left; pick the
        // right piece's α₂ so η''(knot) is continuous given a jumped α₃.
        let left_link = LocalSpanCubic {
            left: knot - 0.6,
            right: knot + 0.6,
            c0: 0.0,
            c1: 0.0,
            c2: 0.08,
            c3: -0.05,
        };
        let right_alpha3 = -0.05_f64 + 0.11; // α₃ jump.
        // η''(knot) continuity:  2α₂ᴸ + 6α₃ᴸ·(knot−leftᴸ) = 2α₂ᴿ + 6α₃ᴿ·(knot−leftᴿ).
        let right_left_coord = knot - 0.4;
        let lhs = 2.0 * left_link.c2 + 6.0 * left_link.c3 * (knot - left_link.left);
        let right_alpha2 = (lhs - 6.0 * right_alpha3 * (knot - right_left_coord)) / 2.0;
        let right_link = LocalSpanCubic {
            left: right_left_coord,
            right: right_left_coord + 0.8,
            c0: 0.0,
            c1: 0.0,
            c2: right_alpha2,
            c3: right_alpha3,
        };
        let (_, _, dc_dbb_left) = link_cubic_second_partials(left_link, a_row, b_row);
        let (_, _, dc_dbb_right) = link_cubic_second_partials(right_link, a_row, b_row);
        // The per-coefficient arrays differ (α₃ jumped)...
        assert!(
            (dc_dbb_left[3] - dc_dbb_right[3]).abs() > 1e-3,
            "α₃ jump must make the raw dc_dbb coefficient arrays differ"
        );
        // ...but the EVALUATED second-order slice at the crossing matches, so the
        // F_bb boundary integrand carries no jump and the flux telescopes to 0.
        let c_bb_left = poly_eval_at(&dc_dbb_left, edge0);
        let c_bb_right = poly_eval_at(&dc_dbb_right, edge0);
        assert!(
            (c_bb_left - c_bb_right).abs() <= 1e-12,
            "second-derivative slope-slope integrand must be CONTINUOUS across the \
             C² knot (telescoping self-flux): left={c_bb_left:.15e} right={c_bb_right:.15e}"
        );
    }
}