fix(optimal_control,risk_metrics): stabilize solvers + statistically sound tests

Five deterministic test failures rooted out (all pre-existing on main):

- mrsjd + regime_switching + hjb_solver: pointwise Jacobi iteration on the
  stationary HJB diverges (sigma^2/dx^2 >> rho, residual -> NaN). Replaced
  with implicit-in-space Kushner-Dupuis upwind discretisation solved by the
  Thomas algorithm (unconditionally stable); removed now-unneeded
  under-relaxation; NaN-safe convergence checks (!(r < tol)).
- hjb_solver: equation had no source term, so V = 0 and the V' = +-1
  boundaries were grid artifacts. Added quadratic tracking payoff and
  singular-control obstacle projection -> symmetric boundaries.
- regime_switching two_regime_model: zero running term made cross-regime
  value comparison meaningless; running payoff f(x) = x makes the
  higher-drift regime strictly more valuable.
- ou_estimator test: stderr(kappa) ~ sqrt(2*kappa/T) was 140% of kappa with
  n=500 and an unseeded rng; now seeded StdRng + T ~ 80y (stderr ~ 22%).
- hurst test: fixture passed alternating +-1 LEVELS; R/S input convention
  is the increment series -> seeded iid +-1 increments.
- hmm doctest: placeholder example executed empty data -> rust,no_run.

Tests: 139/139 (129 lib + 10 doc).
This commit is contained in:
ThotDjehuty
2026-07-07 18:13:53 +02:00
parent 0463382fcb
commit dda201f0d3
6 changed files with 247 additions and 195 deletions
+81 -71
View File
@@ -32,7 +32,6 @@ use crate::optimal_control::{
OptimalControlError, Result,
};
use ndarray::{Array1, Array2};
use rayon::prelude::*;
/// Regime-specific jump parameters
pub struct RegimeJumpParameters {
@@ -207,13 +206,14 @@ impl MRSJDSolver {
if residual < cfg.tolerance {
break;
}
// Relaxation
let omega = 0.5; // More conservative for stability
v = &v * omega + &v_old * (1.0 - omega);
// No under-relaxation: the implicit-in-space solve is
// unconditionally stable, damping only slows convergence.
}
if residual >= cfg.tolerance {
// NOTE: `!(residual < tolerance)` (rather than `residual >= tolerance`)
// also catches NaN residuals, which otherwise slip through both
// comparisons and produce a silently-invalid Ok result.
if !(residual < cfg.tolerance) {
return Err(OptimalControlError::ConvergenceError(format!(
"Failed to converge after {} iterations, residual = {:.2e}",
iterations, residual
@@ -253,80 +253,90 @@ impl MRSJDSolver {
) -> Result<()> {
let cfg = &self.config;
let params = &self.regime_params[regime];
let n = cfg.n_points;
// Compute jump integral for this regime
// Jump inflow λ·Σ_j k_ij v_old_j and outflow mass λ·Σ_j k_ij per node.
// The kernel row sum can be < 1 (jumps leaving the grid are dropped),
// so track it explicitly to keep the scheme conservative.
let lambda = params.jump_intensity;
for i in 0..cfg.n_points {
let mut integral = 0.0;
for j in 0..cfg.n_points {
integral += jump_kernel[[i, j]] * (v_old[[regime, j]] - v_old[[regime, i]]);
let mut jump_mass = vec![0.0_f64; n];
for i in 0..n {
let mut inflow = 0.0;
let mut mass = 0.0;
for j in 0..n {
inflow += jump_kernel[[i, j]] * v_old[[regime, j]];
mass += jump_kernel[[i, j]];
}
jump_int[[regime, i]] = lambda * integral;
jump_int[[regime, i]] = lambda * (inflow - mass * v_old[[regime, i]]);
jump_mass[i] = lambda * mass;
}
// Solve at interior points (parallel)
let updates: Vec<(usize, f64, f64)> = (1..cfg.n_points - 1)
.into_par_iter()
.map(|i| {
let xi = x[i];
// Implicit-in-space solve (KushnerDupuis upwind discretisation).
// The stationary HJB ρv = μ v' + ½σ² v'' + jump + switching + cost
// is rearranged into a diagonally dominant tridiagonal system per
// regime (jumps and regime coupling explicit via v_old), which is
// unconditionally stable — a pointwise Jacobi update diverges here
// because σ²/dx² ≫ ρ.
let mut sub = vec![0.0_f64; n]; // a_i · v_{i-1}
let mut diag = vec![0.0_f64; n]; // b_i · v_i
let mut sup = vec![0.0_f64; n]; // c_i · v_{i+1}
let mut rhs = vec![0.0_f64; n];
// Get values
let v_c = v_old[[regime, i]];
let v_f = v_old[[regime, i + 1]];
let v_b = v_old[[regime, i - 1]];
for i in 1..n - 1 {
let xi = x[i];
let mu = (params.drift)(xi);
let sigma = (params.diffusion)(xi);
let sig2 = sigma * sigma;
let mu_p = mu.max(0.0);
let mu_m = mu.min(0.0);
// Derivatives
let dv_forward = (v_f - v_c) / dx;
let dv_backward = (v_c - v_b) / dx;
let d2v = (v_f - 2.0 * v_c + v_b) / (dx * dx);
// Regime-specific parameters
let mu = (params.drift)(xi);
let sigma = (params.diffusion)(xi);
// Upwind scheme
let drift_term = if mu >= 0.0 {
mu * dv_backward
} else {
mu * dv_forward
};
// Diffusion
let diffusion_term = 0.5 * sigma * sigma * d2v;
// Jump integral
let jump_term = jump_int[[regime, i]];
// Regime switching term
let switching_term: f64 = (0..cfg.n_regimes)
.filter(|&j| j != regime)
.map(|j| q[[regime, j]] * (v_old[[j, i]] - v_c))
.sum();
// Optimal control (placeholder - can be optimized)
let optimal_control =
self.optimize_control_mrsjd(xi, dv_forward, dv_backward, params);
// Running cost
let cost = (params.cost)(xi, optimal_control);
// HJB update
let new_value =
(drift_term + diffusion_term + jump_term + switching_term + cost) / cfg.rho;
(i, new_value, optimal_control)
})
.collect();
// Apply updates
for (i, new_value, optimal_control) in updates {
v[[regime, i]] = new_value;
// Control from the current value gradient (policy-iteration style)
let dv_forward = (v_old[[regime, i + 1]] - v_old[[regime, i]]) / dx;
let dv_backward = (v_old[[regime, i]] - v_old[[regime, i - 1]]) / dx;
let optimal_control = self.optimize_control_mrsjd(xi, dv_forward, dv_backward, params);
u[[regime, i]] = optimal_control;
let cost = (params.cost)(xi, optimal_control);
// Total outflow rate to other regimes
let q_out: f64 = (0..cfg.n_regimes)
.filter(|&j| j != regime)
.map(|j| q[[regime, j]])
.sum();
sub[i] = -(mu_p / dx + 0.5 * sig2 / (dx * dx));
sup[i] = mu_m / dx - 0.5 * sig2 / (dx * dx);
diag[i] = cfg.rho + mu_p / dx - mu_m / dx + sig2 / (dx * dx) + jump_mass[i] + q_out;
// Explicit couplings: jump inflow + other-regime values
let switching_in: f64 = (0..cfg.n_regimes)
.filter(|&j| j != regime)
.map(|j| q[[regime, j]] * v_old[[j, i]])
.sum();
let jump_inflow = jump_int[[regime, i]] + jump_mass[i] * v_old[[regime, i]];
rhs[i] = cost + jump_inflow + switching_in;
}
// Boundaries
v[[regime, 0]] = v[[regime, 1]];
v[[regime, cfg.n_points - 1]] = v[[regime, cfg.n_points - 2]];
// Neumann boundaries: v_0 = v_1, v_{n-1} = v_{n-2}
diag[0] = 1.0;
sup[0] = -1.0;
rhs[0] = 0.0;
sub[n - 1] = -1.0;
diag[n - 1] = 1.0;
rhs[n - 1] = 0.0;
// Thomas algorithm (forward sweep + back substitution)
for i in 1..n {
let w = sub[i] / diag[i - 1];
diag[i] -= w * sup[i - 1];
rhs[i] -= w * rhs[i - 1];
}
v[[regime, n - 1]] = rhs[n - 1] / diag[n - 1];
for i in (0..n - 1).rev() {
v[[regime, i]] = (rhs[i] - sup[i] * v[[regime, i + 1]]) / diag[i];
}
u[[regime, 0]] = u[[regime, 1]];
u[[regime, n - 1]] = u[[regime, n - 2]];
Ok(())
}
@@ -465,7 +475,7 @@ mod tests {
n_regimes: 2,
transition_rates: q,
state_bounds: (-1.0, 3.0),
n_points: 100,
n_points: 200,
rho: 0.05,
transaction_cost: 0.0,
max_iter: 200,