gam 0.3.110

//! `steer_delta` — the **steering primitive with output dosimetry**: the
//! actionable LLM payload of the SAE-manifold machine.
//!
//! # What this computes
//!
//! Given a fitted [`SaeManifoldTerm`] and the per-row output-Fisher
//! [`RowMetric`], a *steering move* is "drive atom `k`'s latent coordinate from
//! `t_from` to `t_to`". The atom's decoder curve `g_k(t) = Φ_k(t) B_k` maps that
//! latent move to an **activation-space delta** — the actual vector you add to
//! the residual stream / reconstruction to realize the move *on the manifold*:
//!
//! ```text
//! δ = a · ( g_k(t_to) − g_k(t_from) )          (the on-manifold move)
//! ```
//!
//! where `a` is the atom's amplitude (how loudly the atom is expressed). This is
//! the thing a downstream consumer adds to a hidden state.
//!
//! # Dosimetry — how big is this push, in nats?
//!
//! The headline number is the **predicted output effect**: how much behavioral
//! change (in nats of KL on the model's output distribution) the move induces.
//! For a locally-quadratic output readout the KL of a parameter move `Δ` is
//! `½ Δᵀ F Δ` with `F` the output-Fisher information — exactly the inner product
//! [`RowMetric`] carries. The dose is the Fisher quadratic form of the move,
//! **integrated along the decoder curve** rather than read only at the endpoints:
//!
//! ```text
//! predicted_nats = ½ ∫_{t_from}^{t_to} a² · g_k'(t)ᵀ M_n g_k'(t) dt
//! ```
//!
//! evaluated in small steps via the per-row pullback / fisher-mass methods. The
//! path integral is the honest dose: it follows the curved surface, so a long arc
//! that doubles back is not under-counted the way a straight endpoint chord would
//! be.
//!
//! # Validity radius — where local linearization stops being trusted
//!
//! A consumer must know *how far* the move can be trusted as a linear push. The
//! **validity radius** is the latent step size at which the path-integrated dose
//! diverges from the straight endpoint quadratic form
//! `½ a² δ̂ᵀ M δ̂` (the local-linear prediction) by more than
//! [`VALIDITY_DIVERGENCE_FRACTION`]. Beyond it the surface has curved enough that
//! the endpoint chord no longer represents the move. We **report** it; we do not
//! silently clip to it.
//!
//! # Off-manifold guard
//!
//! `δ` is, by construction, a chord of the decoder curve, so it should lie in the
//! atom's local tangent/frame at `t_from` (up to second-order curvature). The
//! **off-manifold norm** projects `δ` onto the span of the local decoder tangents
//! `∂g_k/∂t` at `t_from` and reports the residual norm — a self-check that the
//! steering move stays on the learned surface. It is `≈ 0` for small steps and
//! grows with arc curvature; a large value means the requested move left the
//! manifold and the dose number is not to be trusted.
//!
//! # Read-only / no loss contact
//!
//! This module is a **pure read** over the fitted term and the metric. It calls
//! only `g_k(t)` evaluation ([`SaeManifoldAtom`]'s decoder + installed
//! [`SaeBasisEvaluator`]) and the criterion-facing
//! [`RowMetric::fisher_mass`] / [`RowMetric::pullback`]. It never mutates the
//! model, never touches a likelihood / criterion / penalty, and the solver floor
//! `δ` of [`RowMetric`] never enters any number it reports (the fisher-mass /
//! pullback face is `δ`-free, #747).

use ndarray::{Array1, Array2, ArrayView1};

use crate::inference::row_metric::{MetricProvenance, RowMetric};
use crate::inference::structure_evidence::CandidateProbe;
use crate::terms::sae_manifold::SaeManifoldTerm;

/// Number of sub-steps the latent path `[t_from, t_to]` is integrated over for
/// the dosimetry path integral. The decoder curve is smooth, so a modest
/// midpoint-rule grid resolves the arc; fixed (no clock / no adaptivity) so the
/// reported dose is deterministic.
const STEER_PATH_STEPS: usize = 64;

/// The fraction by which the path-integrated dose may diverge from the straight
/// endpoint quadratic form before the move is declared past its validity radius.
/// At `0.1` we trust the linearization while the curved-path dose stays within
/// 10% of the chord dose.
const VALIDITY_DIVERGENCE_FRACTION: f64 = 0.1;

/// Active-mass floor below which a row is "off" for an atom and excluded from the
/// representative-row / amplitude selection. Mirrors `atom_lens::ACTIVE_MASS_FLOOR`.
const ACTIVE_MASS_FLOOR: f64 = 1e-6;

/// The actionable output of a steering query over one atom.
#[derive(Clone, Debug, PartialEq)]
pub struct SteerPlan {
    /// Which atom was steered (index into [`SaeManifoldTerm::atoms`]).
    pub atom: usize,
    /// The atom's name (mirrors [`crate::terms::sae_manifold::SaeManifoldAtom::name`]).
    pub atom_name: String,
    /// The source latent coordinate `t_from` (length = atom's `latent_dim`).
    pub t_from: Vec<f64>,
    /// The target latent coordinate `t_to` (length = atom's `latent_dim`).
    pub t_to: Vec<f64>,
    /// The amplitude `a` the on-manifold move was scaled by (the atom's mean
    /// active assignment mass; `1.0` if the atom is active on no row).
    pub amplitude: f64,
    /// The row whose per-row output-Fisher metric the dose was measured through
    /// (the atom's most-active row; `0` if active nowhere).
    pub measured_row: usize,
    /// **The activation-space delta**: `δ = a · (g_k(t_to) − g_k(t_from))`, a
    /// length-`p` vector in the reconstruction/output space — the actual move to
    /// add to a hidden state.
    pub delta: Array1<f64>,
    /// **DOSIMETRY**: predicted output effect of the move in **nats** of KL,
    /// integrated along the decoder curve through the output-Fisher metric.
    /// `None` when the metric carries no behavioral information (Euclidean
    /// provenance) — the dose is *not available*, not zero.
    pub predicted_nats: Option<f64>,
    /// **VALIDITY RADIUS**: the latent step size (Euclidean norm of the move from
    /// `t_from`) at which the path-integrated dose first diverges from the
    /// straight endpoint quadratic form by more than
    /// [`VALIDITY_DIVERGENCE_FRACTION`]. Equals the full move length when the
    /// linearization is trusted all the way to `t_to`. `None` under a no-behavior
    /// metric (there is no dose to validate).
    pub validity_radius: Option<f64>,
    /// **OFF-MANIFOLD GUARD**: the norm of `δ`'s component outside the span of
    /// the atom's local decoder tangents `∂g_k/∂t` at `t_from`. `≈ 0` by
    /// construction (the move is a chord of the curve); a large value flags a
    /// move that left the learned surface.
    pub off_manifold_norm: f64,
    /// The provenance of the metric the dose was read through, echoed so a
    /// consumer can certify *why* `predicted_nats` is `None` when it is.
    pub metric_provenance: MetricProvenance,
}

/// Build a [`SteerPlan`] for driving atom `atom_k` from `t_from` to `t_to`.
///
/// `model` is the fitted term (read only); `metric` is the per-row output-Fisher
/// inner product the dose is measured through (typically `model.row_metric()`'s
/// own metric, or any metric whose row/output dims match the term). `t_from` and
/// `t_to` are latent coordinates of length `atom.latent_dim`.
///
/// Errors when the atom index is out of range, the coordinate lengths do not
/// match the atom's latent dimension, the atom has no installed
/// [`crate::terms::sae_manifold::SaeBasisEvaluator`] (arbitrary-`t` evaluation
/// requires one), or the metric dimensions do not match the term. Under a
/// Euclidean (no-behavior) metric the geometry is still produced but
/// `predicted_nats` / `validity_radius` degrade to `None`.
pub fn steer_delta(
    model: &SaeManifoldTerm,
    metric: &RowMetric,
    atom_k: usize,
    t_from: &[f64],
    t_to: &[f64],
) -> Result<SteerPlan, String> {
    let k = model.k_atoms();
    if atom_k >= k {
        return Err(format!(
            "steer_delta: atom index {atom_k} out of range (term has {k} atoms)"
        ));
    }
    let atom = &model.atoms[atom_k];
    let d = atom.latent_dim;
    let p = atom.output_dim();
    if t_from.len() != d || t_to.len() != d {
        return Err(format!(
            "steer_delta: t_from/t_to must have length latent_dim={d}; got {} and {}",
            t_from.len(),
            t_to.len()
        ));
    }
    let evaluator = atom.basis_evaluator.as_ref().ok_or_else(|| {
        format!(
            "steer_delta: atom {atom_k} ('{}') has no installed basis evaluator; \
             arbitrary-t decoder evaluation requires one",
            atom.name
        )
    })?;

    // --- amplitude & the row the dose is measured through -------------------
    // The amplitude is the atom's mean active assignment mass (how loudly the
    // atom is expressed), mirroring the presence weighting in `atom_lens`. The
    // measured row is the atom's single most-active row: the per-row metric
    // there is the most representative behavioral inner product for "this atom
    // is on". Both fall back gracefully when the atom is active nowhere.
    let assignments = model.assignment.assignments();
    let n = model.n_obs();
    let mut mass_sum = 0.0_f64;
    let mut active_count = 0.0_f64;
    let mut best_row = 0usize;
    let mut best_mass = f64::NEG_INFINITY;
    for row in 0..n {
        let mass = assignments[[row, atom_k]];
        if mass > best_mass {
            best_mass = mass;
            best_row = row;
        }
        if mass > ACTIVE_MASS_FLOOR {
            mass_sum += mass;
            active_count += 1.0;
        }
    }
    let amplitude = if active_count > 0.0 {
        mass_sum / active_count
    } else {
        1.0
    };

    // --- the on-manifold activation-space delta -----------------------------
    let g_from = decode_at(evaluator.as_ref(), &atom.decoder_coefficients, t_from, p)?;
    let g_to = decode_at(evaluator.as_ref(), &atom.decoder_coefficients, t_to, p)?;
    let mut delta = Array1::<f64>::zeros(p);
    for i in 0..p {
        delta[i] = amplitude * (g_to[i] - g_from[i]);
    }

    // Whether the metric can/does match this term and carries behavior.
    let provenance = metric.provenance();
    let behavior_available =
        metric_carries_behavior(provenance) && metric.n_rows() == n && metric.p_out() == p;

    // --- off-manifold guard -------------------------------------------------
    // Project δ onto the span of the local decoder tangents ∂g_k/∂t and report
    // the residual norm. The tangents are evaluated at the move's MIDPOINT, not
    // at t_from: the chord of a curve is symmetric about its midpoint, so its
    // component transverse to the midpoint tangent is the true second-order
    // sagitta (`O(‖Δt‖²)`), whereas the endpoint tangent differs from the chord
    // direction already at first order. Measuring against the midpoint frame is
    // therefore the honest "did the move stay on the surface" self-check: it is
    // `≈ 0` for an on-manifold move and grows only with genuine arc curvature.
    let mut t_mid = vec![0.0_f64; d];
    for a in 0..d {
        t_mid[a] = 0.5 * (t_from[a] + t_to[a]);
    }
    let tangents =
        decode_tangents_at(evaluator.as_ref(), &atom.decoder_coefficients, &t_mid, p, d)?;
    let off_manifold_norm = off_manifold_residual_norm(&tangents, delta.view());

    // --- dosimetry: path-integrated Fisher dose -----------------------------
    let (predicted_nats, validity_radius) = if !behavior_available {
        (None, None)
    } else {
        let ctx = SteerContext {
            evaluator: evaluator.as_ref(),
            decoder: &atom.decoder_coefficients,
            metric,
            row: best_row,
            p,
            d,
            amplitude,
        };
        let dose = path_integrated_dose(&ctx, t_from, t_to)?;
        let radius = validity_radius(&ctx, t_from, t_to)?;
        (Some(dose), Some(radius))
    };

    Ok(SteerPlan {
        atom: atom_k,
        atom_name: atom.name.clone(),
        t_from: t_from.to_vec(),
        t_to: t_to.to_vec(),
        amplitude,
        measured_row: best_row,
        delta,
        predicted_nats,
        validity_radius,
        off_manifold_norm,
        metric_provenance: provenance,
    })
}

/// The model's predicted output-mean response to an applied activation push
/// `δ`, under the LOCAL-LINEAR reading of its fitted surface: the projection
/// of `δ` onto the span of atom `atom_k`'s decoder tangents `∂g_k/∂t` at the
/// operating point `t_at`. A dictionary "predicts" exactly the component of a
/// push it can carry along its learned surface; the transverse component is
/// off-manifold and predicted to die (this is the same local model the
/// off-manifold guard and the dosimetry chord trust, used in the same radius).
///
/// This is `μ(δ)` for the design loop of
/// [`crate::inference::structure_evidence`]: two structural hypotheses about
/// the same activations (e.g. "one curved atom" vs "two flat atoms") are two
/// fitted terms whose tangent spans differ, so they predict DIFFERENT
/// responses to the same probe — and that disagreement, in the output-Fisher
/// metric, is what `select_probe_by_expected_evidence` maximizes.
pub fn predicted_response(
    model: &SaeManifoldTerm,
    atom_k: usize,
    t_at: &[f64],
    delta: ArrayView1<'_, f64>,
) -> Result<Array1<f64>, String> {
    let k = model.k_atoms();
    if atom_k >= k {
        return Err(format!(
            "predicted_response: atom index {atom_k} out of range (term has {k} atoms)"
        ));
    }
    let atom = &model.atoms[atom_k];
    let d = atom.latent_dim;
    let p = atom.output_dim();
    if t_at.len() != d {
        return Err(format!(
            "predicted_response: t_at must have length latent_dim={d}; got {}",
            t_at.len()
        ));
    }
    if delta.len() != p {
        return Err(format!(
            "predicted_response: delta must have length output_dim={p}; got {}",
            delta.len()
        ));
    }
    let evaluator = atom.basis_evaluator.as_ref().ok_or_else(|| {
        format!(
            "predicted_response: atom {atom_k} ('{}') has no installed basis evaluator",
            atom.name
        )
    })?;
    let tangents = decode_tangents_at(evaluator.as_ref(), &atom.decoder_coefficients, t_at, p, d)?;
    Ok(project_onto_tangent_span(&tangents, delta))
}

/// Build the [`CandidateProbe`] for one contested structural claim from the
/// two hypotheses' FITTED dictionaries — the bridge that closes the design
/// loop (probe → dosimetry → likelihood → absorb): the probe's δ comes from a
/// [`SteerPlan`] (so the steering primitive's validity radius and dosimetry
/// govern it), and each hypothesis predicts its own response via
/// [`predicted_response`] at its own operating point (its atom + latent
/// coordinate representing the same activations — under "one curved atom vs
/// two flat atoms" the hypotheses do not even share an atom index, hence the
/// per-hypothesis anchors). Feed the result to
/// `structure_evidence::select_probe_by_expected_evidence` /
/// `plan_probe_for_contested_claim` with the #980 output-Fisher metric.
pub struct HypothesisAnchor<'a> {
    pub model: &'a SaeManifoldTerm,
    /// The atom whose local surface represents the probed activations under
    /// this hypothesis.
    pub atom: usize,
    /// The latent operating point on that atom.
    pub t_at: &'a [f64],
}

/// See [`HypothesisAnchor`].
pub fn candidate_probe_from_hypotheses(
    plan: &SteerPlan,
    null_hypothesis: HypothesisAnchor<'_>,
    alt_hypothesis: HypothesisAnchor<'_>,
) -> Result<CandidateProbe, String> {
    let predicted_mean_null = predicted_response(
        null_hypothesis.model,
        null_hypothesis.atom,
        null_hypothesis.t_at,
        plan.delta.view(),
    )?;
    let predicted_mean_alt = predicted_response(
        alt_hypothesis.model,
        alt_hypothesis.atom,
        alt_hypothesis.t_at,
        plan.delta.view(),
    )?;
    Ok(CandidateProbe {
        delta: plan.delta.clone(),
        predicted_mean_null,
        predicted_mean_alt,
    })
}

/// Does this provenance carry behavioral (output-Fisher) information? Euclidean
/// is the isotropic activation-only path and carries none; the factored
/// provenances do. (Mirrors `atom_lens::metric_carries_behavior`.)
fn metric_carries_behavior(p: MetricProvenance) -> bool {
    match p {
        MetricProvenance::Euclidean => false,
        MetricProvenance::OutputFisher { .. } | MetricProvenance::WhitenedStructured { .. } => true,
    }
}

/// Evaluate the decoder output `g_k(t) = Φ_k(t) B_k ∈ ℝ^p` at an arbitrary
/// latent coordinate `t` (length `d`) via the atom's installed evaluator.
fn decode_at(
    evaluator: &dyn crate::terms::sae_manifold::SaeBasisEvaluator,
    decoder: &Array2<f64>,
    t: &[f64],
    p: usize,
) -> Result<Array1<f64>, String> {
    let d = t.len();
    let coords = Array2::from_shape_vec((1, d), t.to_vec())
        .map_err(|e| format!("steer_delta::decode_at: coord shape: {e}"))?;
    let (phi, _jet) = evaluator.evaluate(coords.view())?;
    let m = decoder.nrows();
    if phi.ncols() != m {
        return Err(format!(
            "steer_delta::decode_at: evaluator returned {} basis cols but decoder has {m} rows",
            phi.ncols()
        ));
    }
    let mut g = Array1::<f64>::zeros(p);
    for basis_col in 0..m {
        let phi_v = phi[[0, basis_col]];
        if phi_v == 0.0 {
            continue;
        }
        for out_col in 0..p {
            g[out_col] += phi_v * decoder[[basis_col, out_col]];
        }
    }
    Ok(g)
}

/// Evaluate the decoder tangents `∂g_k/∂t_a = Φ_k'(t) B_k ∈ ℝ^p`, one per latent
/// axis `a ∈ 0..d`, at an arbitrary latent coordinate `t`. Returned as a
/// `(p × d)` matrix whose column `a` is the tangent along axis `a`.
fn decode_tangents_at(
    evaluator: &dyn crate::terms::sae_manifold::SaeBasisEvaluator,
    decoder: &Array2<f64>,
    t: &[f64],
    p: usize,
    d: usize,
) -> Result<Array2<f64>, String> {
    let coords = Array2::from_shape_vec((1, d), t.to_vec())
        .map_err(|e| format!("steer_delta::decode_tangents_at: coord shape: {e}"))?;
    let (_phi, jet) = evaluator.evaluate(coords.view())?;
    let m = decoder.nrows();
    if jet.dim() != (1, m, d) {
        return Err(format!(
            "steer_delta::decode_tangents_at: evaluator jet {:?} != (1, {m}, {d})",
            jet.dim()
        ));
    }
    let mut tang = Array2::<f64>::zeros((p, d));
    for axis in 0..d {
        for basis_col in 0..m {
            let dphi = jet[[0, basis_col, axis]];
            if dphi == 0.0 {
                continue;
            }
            for out_col in 0..p {
                tang[[out_col, axis]] += dphi * decoder[[basis_col, out_col]];
            }
        }
    }
    Ok(tang)
}

/// Least-squares projection of `δ` onto the span of the local tangents
/// (columns of `tangents`, shape `p × d`): `δ̂ = T (TᵀT)⁻¹ Tᵀ δ` via a small
/// `d × d` Gram solve (with a tiny diagonal jitter to absorb a rank-deficient
/// tangent frame; the jitter only shrinks the projection, never inflates it).
fn project_onto_tangent_span(tangents: &Array2<f64>, delta: ArrayView1<'_, f64>) -> Array1<f64> {
    let p = tangents.nrows();
    let d = tangents.ncols();
    if d == 0 {
        return Array1::<f64>::zeros(p);
    }
    // Gram = TᵀT (d × d) and rhs = Tᵀδ (d).
    let mut gram = Array2::<f64>::zeros((d, d));
    let mut rhs = Array1::<f64>::zeros(d);
    for a in 0..d {
        let mut r = 0.0_f64;
        for i in 0..p {
            r += tangents[[i, a]] * delta[i];
        }
        rhs[a] = r;
        for b in a..d {
            let mut acc = 0.0_f64;
            for i in 0..p {
                acc += tangents[[i, a]] * tangents[[i, b]];
            }
            gram[[a, b]] = acc;
            gram[[b, a]] = acc;
        }
    }
    let trace: f64 = (0..d).map(|a| gram[[a, a]]).sum();
    let jitter = if trace > 0.0 { 1e-12 * trace } else { 1e-12 };
    for a in 0..d {
        gram[[a, a]] += jitter;
    }
    let coeffs = solve_spd_small(&gram, &rhs);
    let mut proj = Array1::<f64>::zeros(p);
    for i in 0..p {
        for a in 0..d {
            proj[i] += tangents[[i, a]] * coeffs[a];
        }
    }
    proj
}

/// Norm of `δ`'s component orthogonal to the span of the local tangents:
/// `‖δ − δ̂‖` with `δ̂` the [`project_onto_tangent_span`] projection.
fn off_manifold_residual_norm(tangents: &Array2<f64>, delta: ArrayView1<'_, f64>) -> f64 {
    let proj = project_onto_tangent_span(tangents, delta);
    let mut res_sq = 0.0_f64;
    for i in 0..delta.len() {
        let r = delta[i] - proj[i];
        res_sq += r * r;
    }
    res_sq.max(0.0).sqrt()
}

/// Tiny symmetric-positive-definite solve via Cholesky for the `d × d` tangent
/// Gram (`d` is the atom's latent dim, typically 1–3). Falls back to the bare rhs
/// if the factorization fails (a fully degenerate frame), which only inflates the
/// reported off-manifold residual — never deflates it.
fn solve_spd_small(gram: &Array2<f64>, rhs: &Array1<f64>) -> Array1<f64> {
    let d = gram.nrows();
    // Cholesky L LᵀT = gram.
    let mut l = Array2::<f64>::zeros((d, d));
    for i in 0..d {
        for j in 0..=i {
            let mut sum = gram[[i, j]];
            for k in 0..j {
                sum -= l[[i, k]] * l[[j, k]];
            }
            if i == j {
                if sum <= 0.0 {
                    return Array1::<f64>::zeros(d);
                }
                l[[i, j]] = sum.sqrt();
            } else {
                l[[i, j]] = sum / l[[j, j]];
            }
        }
    }
    // Forward solve L y = rhs.
    let mut y = Array1::<f64>::zeros(d);
    for i in 0..d {
        let mut sum = rhs[i];
        for k in 0..i {
            sum -= l[[i, k]] * y[k];
        }
        y[i] = sum / l[[i, i]];
    }
    // Back solve Lᵀ x = y.
    let mut x = Array1::<f64>::zeros(d);
    for i in (0..d).rev() {
        let mut sum = y[i];
        for k in (i + 1)..d {
            sum -= l[[k, i]] * x[k];
        }
        x[i] = sum / l[[i, i]];
    }
    x
}

/// The fixed geometry of one steering query, bundled so the dose integrator and
/// its helpers take a single context rather than a long argument list.
struct SteerContext<'a> {
    evaluator: &'a dyn crate::terms::sae_manifold::SaeBasisEvaluator,
    decoder: &'a Array2<f64>,
    metric: &'a RowMetric,
    /// The row whose per-row metric the dose is measured through.
    row: usize,
    /// Output dimension `p`.
    p: usize,
    /// Latent dimension `d`.
    d: usize,
    /// Amplitude `a` the move is scaled by.
    amplitude: f64,
}

/// Path-integrated Fisher dose
/// `½ a² ∫ g_k'(t)ᵀ M g_k'(t) dt` along the straight latent segment
/// `t(τ) = t_from + τ (t_to − t_from)`, `τ ∈ [0, 1]`, by the midpoint rule over
/// [`STEER_PATH_STEPS`] sub-steps.
///
/// The local quadratic `g'(t)ᵀ M g'(t)` is the [`RowMetric::pullback`] of the
/// per-axis decoder tangents contracted with the latent velocity `Δt`, so this
/// uses only the criterion-facing pullback (no loss / no solver floor).
fn path_integrated_dose(
    ctx: &SteerContext<'_>,
    t_from: &[f64],
    t_to: &[f64],
) -> Result<f64, String> {
    let d = ctx.d;
    let p = ctx.p;
    let steps = STEER_PATH_STEPS;
    let dtau = 1.0 / steps as f64;
    // Latent velocity Δt (constant along the straight segment).
    let mut dt = vec![0.0_f64; d];
    for a in 0..d {
        dt[a] = t_to[a] - t_from[a];
    }
    let mut acc = 0.0_f64;
    let amp2 = ctx.amplitude * ctx.amplitude;
    for s in 0..steps {
        // Midpoint of sub-step s in τ, mapped to a latent coordinate.
        let tau_mid = (s as f64 + 0.5) * dtau;
        let mut t_mid = vec![0.0_f64; d];
        for a in 0..d {
            t_mid[a] = t_from[a] + tau_mid * dt[a];
        }
        // Decoder tangents at the midpoint: ∂g/∂t_a, columns of a (p × d) matrix.
        let tang = decode_tangents_at(ctx.evaluator, ctx.decoder, &t_mid, p, d)?;
        // The pulled-back metric at this point is g_{ab} = (∂g/∂t)ᵀ M (∂g/∂t),
        // the d × d local inner product of latent motion *in output-Fisher
        // units*. We form it through the criterion-facing `RowMetric::pullback`
        // (which never materializes the p × p M and never sees the solver δ),
        // then contract the latent velocity Δt twice: the squared output-Fisher
        // speed along the path is Δtᵀ g Δt. The decoder Jacobian is passed flat
        // row-major (J[i, a] = j_row[i * d + a]) as `pullback` expects.
        let mut j_row = vec![0.0_f64; p * d];
        for i in 0..p {
            for a in 0..d {
                j_row[i * d + a] = tang[[i, a]];
            }
        }
        let g_ab = ctx.metric.pullback(ctx.row, &j_row, d);
        let mut speed_sq = 0.0_f64;
        for a in 0..d {
            for b in 0..d {
                speed_sq += dt[a] * g_ab[[a, b]] * dt[b];
            }
        }
        acc += 0.5 * amp2 * speed_sq * dtau;
    }
    Ok(acc)
}

/// The validity radius: the latent step length (Euclidean distance from
/// `t_from`) at which **local linearization stops being trusted**.
///
/// Linearizing the steering move means predicting the output effect of a prefix
/// step `τ·Δt` from the initial tangent alone: the first-order output move is
/// `δ_lin(τ) = a · (∂g/∂t|_{t_from}) · (τ Δt)`, whose output-Fisher KL is the
/// quadratic form `½ ‖δ_lin(τ)‖²_M = τ² · ½ a² ‖∂g/∂t·Δt‖²_M`. The **true**
/// effect of that prefix is the chord quadratic form of the *actual* curved
/// output move `½ a² ‖g(t_from + τΔt) − g(t_from)‖²_M`.
///
/// The radius is the chord length `τ* · ‖Δt‖` at the first prefix `τ*` where the
/// true chord KL diverges from the linear prediction by more than
/// [`VALIDITY_DIVERGENCE_FRACTION`] (relative to the linear prediction). This is
/// pure surface curvature: on a flat decoder the two agree for every `τ` and the
/// radius is the whole move. If the metric kills the tangent (no linear effect to
/// validate), the move is trusted to its full length.
fn validity_radius(ctx: &SteerContext<'_>, t_from: &[f64], t_to: &[f64]) -> Result<f64, String> {
    let d = ctx.d;
    let p = ctx.p;
    let full_len: f64 = t_from
        .iter()
        .zip(t_to.iter())
        .map(|(&a, &b)| (b - a) * (b - a))
        .sum::<f64>()
        .sqrt();
    if full_len == 0.0 {
        return Ok(0.0);
    }
    let mut dt = vec![0.0_f64; d];
    for a in 0..d {
        dt[a] = t_to[a] - t_from[a];
    }
    let amp = ctx.amplitude;

    // Initial-tangent linear output move per unit τ: v0 = (∂g/∂t|_{t_from}) Δt.
    let tang0 = decode_tangents_at(ctx.evaluator, ctx.decoder, t_from, p, d)?;
    let mut v0 = Array1::<f64>::zeros(p);
    for i in 0..p {
        let mut acc = 0.0_f64;
        for a in 0..d {
            acc += tang0[[i, a]] * dt[a];
        }
        v0[i] = acc;
    }
    // ½ a² ‖v0‖²_M — the per-τ² linear KL coefficient.
    let lin_coeff = 0.5 * amp * amp * ctx.metric.fisher_mass(ctx.row, v0.view());
    // No linear effect to validate against ⇒ trust the full move.
    if !(lin_coeff > 0.0) {
        return Ok(full_len);
    }

    let g_from = decode_at(ctx.evaluator, ctx.decoder, t_from, p)?;
    let steps = STEER_PATH_STEPS;
    for s in 0..steps {
        let tau = (s as f64 + 1.0) / steps as f64;
        let mut t_mid = vec![0.0_f64; d];
        for a in 0..d {
            t_mid[a] = t_from[a] + tau * dt[a];
        }
        let g_tau = decode_at(ctx.evaluator, ctx.decoder, &t_mid, p)?;
        let mut chord = Array1::<f64>::zeros(p);
        for i in 0..p {
            chord[i] = amp * (g_tau[i] - g_from[i]);
        }
        // True chord KL of the prefix, and the linear prediction τ²·lin_coeff.
        let chord_kl = 0.5 * ctx.metric.fisher_mass(ctx.row, chord.view());
        let lin_kl = tau * tau * lin_coeff;
        let rel = (chord_kl - lin_kl).abs() / lin_kl;
        if rel > VALIDITY_DIVERGENCE_FRACTION {
            return Ok(tau * full_len);
        }
    }
    Ok(full_len)
}