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oxiphysics_core/
numerical_methods.rs

1#![allow(clippy::needless_range_loop)]
2// Copyright 2026 COOLJAPAN OU (Team KitaSan)
3// SPDX-License-Identifier: Apache-2.0
4
5//! Numerical methods: root finding, ODE solvers, BVP, finite differences,
6//! numerical differentiation, quadrature, matrix decompositions, eigensolvers,
7//! continuation methods, and bifurcation detection.
8
9#![allow(dead_code)]
10#![allow(unused_imports)]
11#![allow(clippy::too_many_arguments)]
12
13use std::f64::consts::{FRAC_1_SQRT_2, PI};
14
15// ---------------------------------------------------------------------------
16// Root finding
17// ---------------------------------------------------------------------------
18
19/// Result of a root-finding computation.
20#[derive(Debug, Clone)]
21pub struct RootResult {
22    /// Estimated root
23    pub root: f64,
24    /// Function value at root
25    pub f_val: f64,
26    /// Number of iterations
27    pub iterations: usize,
28    /// Converged?
29    pub converged: bool,
30}
31
32/// Newton-Raphson root finding.
33///
34/// Finds `x` such that `f(x) = 0` given an initial guess and derivative `df`.
35pub fn newton_raphson<F, DF>(f: F, df: DF, x0: f64, tol: f64, max_iter: usize) -> RootResult
36where
37    F: Fn(f64) -> f64,
38    DF: Fn(f64) -> f64,
39{
40    let mut x = x0;
41    for i in 0..max_iter {
42        let fx = f(x);
43        if fx.abs() < tol {
44            return RootResult {
45                root: x,
46                f_val: fx,
47                iterations: i,
48                converged: true,
49            };
50        }
51        let dfx = df(x);
52        if dfx.abs() < 1e-15 {
53            break;
54        }
55        x -= fx / dfx;
56    }
57    let fx = f(x);
58    RootResult {
59        root: x,
60        f_val: fx,
61        iterations: max_iter,
62        converged: fx.abs() < tol,
63    }
64}
65
66/// Secant method for root finding (no derivative required).
67pub fn secant_method<F>(f: F, x0: f64, x1: f64, tol: f64, max_iter: usize) -> RootResult
68where
69    F: Fn(f64) -> f64,
70{
71    let mut xa = x0;
72    let mut xb = x1;
73    let mut fa = f(xa);
74    for i in 0..max_iter {
75        let fb = f(xb);
76        if fb.abs() < tol {
77            return RootResult {
78                root: xb,
79                f_val: fb,
80                iterations: i,
81                converged: true,
82            };
83        }
84        if (fb - fa).abs() < 1e-15 {
85            break;
86        }
87        let xc = xb - fb * (xb - xa) / (fb - fa);
88        xa = xb;
89        fa = fb;
90        xb = xc;
91    }
92    let fval = f(xb);
93    RootResult {
94        root: xb,
95        f_val: fval,
96        iterations: max_iter,
97        converged: fval.abs() < tol,
98    }
99}
100
101/// Brent's method (Brentq) for robust bracketed root finding.
102///
103/// Requires `f(a)` and `f(b)` to have opposite signs.
104pub fn brentq<F>(f: F, a: f64, b: f64, tol: f64, max_iter: usize) -> RootResult
105where
106    F: Fn(f64) -> f64,
107{
108    let mut a = a;
109    let mut b = b;
110    let mut fa = f(a);
111    let fb = f(b);
112    if fa * fb > 0.0 {
113        return RootResult {
114            root: a,
115            f_val: fa,
116            iterations: 0,
117            converged: false,
118        };
119    }
120    let mut c = a;
121    let mut fc = fa;
122    let mut d = b - a;
123    let mut e = d;
124    for i in 0..max_iter {
125        if fb * fc > 0.0 {
126            c = a;
127            fc = fa;
128            d = b - a;
129            e = d;
130        }
131        if fc.abs() < fb.abs() {
132            a = b;
133            b = c;
134            c = a;
135            fa = fb;
136            let fb_new = fc;
137            fc = fa;
138            let _ = fb_new;
139        }
140        let tol1 = 2.0 * f64::EPSILON * b.abs() + tol / 2.0;
141        let xm = (c - b) / 2.0;
142        if xm.abs() <= tol1 || fb.abs() < tol {
143            return RootResult {
144                root: b,
145                f_val: f(b),
146                iterations: i,
147                converged: true,
148            };
149        }
150        if e.abs() >= tol1 && fa.abs() > fb.abs() {
151            let s = fb / fa;
152            let p;
153            let q;
154            if (a - c).abs() < 1e-15 {
155                p = 2.0 * xm * s;
156                q = 1.0 - s;
157            } else {
158                let r = fb / fc;
159                let s2 = fb / fa;
160                p = s2 * (2.0 * xm * r * (r - s2) - (b - a) * (s2 - 1.0));
161                q = (r - 1.0) * (s2 - 1.0) * (r - s2);
162                let _ = s;
163                let _ = p;
164                let _ = q;
165                let p2 = s2 * (2.0 * xm * r * (r - s2) - (b - a) * (s2 - 1.0));
166                let q2 = (r - 1.0) * (s2 - 1.0) * (r - s2);
167                if p2 > 0.0 {
168                    d = p2 / q2.abs();
169                } else {
170                    d = -p2 / q2.abs();
171                }
172                if 2.0 * d < 3.0 * xm - tol1.abs() * (if xm >= 0.0 { 1.0 } else { -1.0 }) {
173                    e = d;
174                } else {
175                    d = xm;
176                    e = d;
177                }
178                let _ = p;
179                let _ = q;
180            }
181            let _ = p;
182            let _ = q;
183        } else {
184            d = xm;
185            e = d;
186        }
187        a = b;
188        fa = f(b);
189        if d.abs() > tol1 {
190            b += d;
191        } else if xm >= 0.0 {
192            b += tol1;
193        } else {
194            b -= tol1;
195        }
196        let fb_new = f(b);
197        let _ = fb_new;
198        if fb.abs() < tol {
199            return RootResult {
200                root: b,
201                f_val: f(b),
202                iterations: i,
203                converged: true,
204            };
205        }
206    }
207    RootResult {
208        root: b,
209        f_val: f(b),
210        iterations: max_iter,
211        converged: false,
212    }
213}
214
215/// Bisection method (guaranteed convergence on bracket).
216pub fn bisect<F>(f: F, mut a: f64, mut b: f64, tol: f64, max_iter: usize) -> RootResult
217where
218    F: Fn(f64) -> f64,
219{
220    let mut fa = f(a);
221    for i in 0..max_iter {
222        let mid = (a + b) / 2.0;
223        let fmid = f(mid);
224        if fmid.abs() < tol || (b - a) / 2.0 < tol {
225            return RootResult {
226                root: mid,
227                f_val: fmid,
228                iterations: i,
229                converged: true,
230            };
231        }
232        if fa * fmid < 0.0 {
233            b = mid;
234        } else {
235            a = mid;
236            fa = fmid;
237        }
238    }
239    let mid = (a + b) / 2.0;
240    RootResult {
241        root: mid,
242        f_val: f(mid),
243        iterations: max_iter,
244        converged: false,
245    }
246}
247
248// ---------------------------------------------------------------------------
249// ODE solvers
250// ---------------------------------------------------------------------------
251
252/// Euler's method for ODEs: dy/dt = f(t, y).
253///
254/// Returns (time, state) pairs.
255pub fn euler_ode<F>(f: F, t0: f64, y0: Vec<f64>, t_end: f64, dt: f64) -> Vec<(f64, Vec<f64>)>
256where
257    F: Fn(f64, &[f64]) -> Vec<f64>,
258{
259    let mut t = t0;
260    let mut y = y0;
261    let mut result = vec![(t, y.clone())];
262    while t < t_end - dt * 0.5 {
263        let dy = f(t, &y);
264        for i in 0..y.len() {
265            y[i] += dy[i] * dt;
266        }
267        t += dt;
268        result.push((t, y.clone()));
269    }
270    result
271}
272
273/// Runge-Kutta 2nd order (Heun's method).
274pub fn rk2<F>(f: F, t0: f64, y0: Vec<f64>, t_end: f64, dt: f64) -> Vec<(f64, Vec<f64>)>
275where
276    F: Fn(f64, &[f64]) -> Vec<f64>,
277{
278    let mut t = t0;
279    let mut y = y0;
280    let mut result = vec![(t, y.clone())];
281    while t < t_end - dt * 0.5 {
282        let k1 = f(t, &y);
283        let y_pred: Vec<f64> = y.iter().zip(k1.iter()).map(|(yi, k)| yi + k * dt).collect();
284        let k2 = f(t + dt, &y_pred);
285        for i in 0..y.len() {
286            y[i] += (k1[i] + k2[i]) * dt / 2.0;
287        }
288        t += dt;
289        result.push((t, y.clone()));
290    }
291    result
292}
293
294/// Classic 4th-order Runge-Kutta.
295pub fn rk4<F>(f: F, t0: f64, y0: Vec<f64>, t_end: f64, dt: f64) -> Vec<(f64, Vec<f64>)>
296where
297    F: Fn(f64, &[f64]) -> Vec<f64>,
298{
299    let mut t = t0;
300    let mut y = y0;
301    let mut result = vec![(t, y.clone())];
302    while t < t_end - dt * 0.5 {
303        let k1 = f(t, &y);
304        let y2: Vec<f64> = y
305            .iter()
306            .zip(k1.iter())
307            .map(|(yi, k)| yi + k * dt / 2.0)
308            .collect();
309        let k2 = f(t + dt / 2.0, &y2);
310        let y3: Vec<f64> = y
311            .iter()
312            .zip(k2.iter())
313            .map(|(yi, k)| yi + k * dt / 2.0)
314            .collect();
315        let k3 = f(t + dt / 2.0, &y3);
316        let y4: Vec<f64> = y.iter().zip(k3.iter()).map(|(yi, k)| yi + k * dt).collect();
317        let k4 = f(t + dt, &y4);
318        for i in 0..y.len() {
319            y[i] += (k1[i] + 2.0 * k2[i] + 2.0 * k3[i] + k4[i]) * dt / 6.0;
320        }
321        t += dt;
322        result.push((t, y.clone()));
323    }
324    result
325}
326
327/// Dormand-Prince RK45 adaptive step integrator.
328///
329/// Returns (t, y) pairs with local error control.
330#[derive(Debug, Clone)]
331pub struct Rk45State {
332    /// Current time
333    pub t: f64,
334    /// Current state
335    pub y: Vec<f64>,
336    /// Step size
337    pub h: f64,
338    /// Tolerance
339    pub rtol: f64,
340    /// Absolute tolerance
341    pub atol: f64,
342}
343
344/// Dormand-Prince RK45 Butcher tableau coefficients.
345const RK45_A: [[f64; 5]; 6] = [
346    [0.0, 0.0, 0.0, 0.0, 0.0],
347    [1.0 / 5.0, 0.0, 0.0, 0.0, 0.0],
348    [3.0 / 40.0, 9.0 / 40.0, 0.0, 0.0, 0.0],
349    [44.0 / 45.0, -56.0 / 15.0, 32.0 / 9.0, 0.0, 0.0],
350    [
351        19372.0 / 6561.0,
352        -25360.0 / 2187.0,
353        64448.0 / 6561.0,
354        -212.0 / 729.0,
355        0.0,
356    ],
357    [
358        9017.0 / 3168.0,
359        -355.0 / 33.0,
360        46732.0 / 5247.0,
361        49.0 / 176.0,
362        -5103.0 / 18656.0,
363    ],
364];
365const RK45_C: [f64; 6] = [0.0, 1.0 / 5.0, 3.0 / 10.0, 4.0 / 5.0, 8.0 / 9.0, 1.0];
366const RK45_B5: [f64; 6] = [
367    35.0 / 384.0,
368    0.0,
369    500.0 / 1113.0,
370    125.0 / 192.0,
371    -2187.0 / 6784.0,
372    11.0 / 84.0,
373];
374const RK45_E: [f64; 6] = [
375    71.0 / 57600.0,
376    0.0,
377    -71.0 / 16695.0,
378    71.0 / 1920.0,
379    -17253.0 / 339200.0,
380    22.0 / 525.0,
381];
382
383/// Perform one RK45 step. Returns (y_new, error_estimate).
384pub fn rk45_step<F>(f: &F, t: f64, y: &[f64], h: f64) -> (Vec<f64>, Vec<f64>)
385where
386    F: Fn(f64, &[f64]) -> Vec<f64>,
387{
388    let n = y.len();
389    let mut k = Vec::with_capacity(6);
390    k.push(f(t, y));
391    for stage in 1..6 {
392        let t_s = t + RK45_C[stage] * h;
393        let y_s: Vec<f64> = (0..n)
394            .map(|i| y[i] + h * (0..stage).map(|j| RK45_A[stage][j] * k[j][i]).sum::<f64>())
395            .collect();
396        k.push(f(t_s, &y_s));
397    }
398    let y_new: Vec<f64> = (0..n)
399        .map(|i| y[i] + h * (0..6).map(|j| RK45_B5[j] * k[j][i]).sum::<f64>())
400        .collect();
401    let err: Vec<f64> = (0..n)
402        .map(|i| h * (0..6).map(|j| RK45_E[j] * k[j][i]).sum::<f64>())
403        .collect();
404    (y_new, err)
405}
406
407/// Adaptive RK45 integrator.
408pub fn rk45_adaptive<F>(
409    f: F,
410    t0: f64,
411    y0: Vec<f64>,
412    t_end: f64,
413    rtol: f64,
414    atol: f64,
415) -> Vec<(f64, Vec<f64>)>
416where
417    F: Fn(f64, &[f64]) -> Vec<f64>,
418{
419    let mut t = t0;
420    let mut y = y0.clone();
421    let mut h = (t_end - t0) / 100.0;
422    let mut result = vec![(t, y.clone())];
423    let max_steps = 100_000;
424    let mut steps = 0;
425    while t < t_end - 1e-12 && steps < max_steps {
426        h = h.min(t_end - t);
427        let (y_new, err) = rk45_step(&f, t, &y, h);
428        // Error norm
429        let err_norm = {
430            let n = y.len() as f64;
431            let sum: f64 = err
432                .iter()
433                .zip(y.iter())
434                .zip(y_new.iter())
435                .map(|((e, yi), yi_new)| {
436                    let sc = atol + rtol * yi.abs().max(yi_new.abs());
437                    (e / sc).powi(2)
438                })
439                .sum();
440            (sum / n).sqrt()
441        };
442        if err_norm <= 1.0 {
443            t += h;
444            y = y_new;
445            result.push((t, y.clone()));
446            // Increase step
447            let factor = 0.9 * err_norm.powf(-0.2);
448            h *= factor.clamp(0.1, 5.0);
449        } else {
450            // Decrease step
451            let factor = 0.9 * err_norm.powf(-0.2);
452            h *= factor.clamp(0.1, 1.0);
453        }
454        steps += 1;
455    }
456    result
457}
458
459// ---------------------------------------------------------------------------
460// BVP shooting method
461// ---------------------------------------------------------------------------
462
463/// Solve a second-order BVP y''=f(x,y,y') with y(a)=ya, y(b)=yb.
464///
465/// Uses single shooting with Newton iteration on the initial slope.
466pub fn bvp_shoot<F>(
467    f: F,
468    a: f64,
469    b: f64,
470    ya: f64,
471    yb: f64,
472    s0: f64,
473    n_steps: usize,
474    tol: f64,
475) -> Vec<(f64, f64)>
476where
477    F: Fn(f64, f64, f64) -> f64,
478{
479    let shoot = |s: f64| -> Vec<(f64, f64)> {
480        let dt = (b - a) / n_steps as f64;
481        let mut x = a;
482        let mut y = ya;
483        let mut dy = s;
484        let mut path = vec![(x, y)];
485        for _ in 0..n_steps {
486            let k1y = dy;
487            let k1dy = f(x, y, dy);
488            let k2y = dy + k1dy * dt / 2.0;
489            let k2dy = f(x + dt / 2.0, y + k1y * dt / 2.0, dy + k1dy * dt / 2.0);
490            let k3y = dy + k2dy * dt / 2.0;
491            let k3dy = f(x + dt / 2.0, y + k2y * dt / 2.0, dy + k2dy * dt / 2.0);
492            let k4y = dy + k3dy * dt;
493            let k4dy = f(x + dt, y + k3y * dt, dy + k3dy * dt);
494            y += (k1y + 2.0 * k2y + 2.0 * k3y + k4y) * dt / 6.0;
495            dy += (k1dy + 2.0 * k2dy + 2.0 * k3dy + k4dy) * dt / 6.0;
496            x += dt;
497            path.push((x, y));
498        }
499        path
500    };
501    let boundary_residual = |s: f64| -> f64 {
502        let path = shoot(s);
503        path.last().map(|(_, y)| *y).unwrap_or(0.0) - yb
504    };
505    // Newton on s
506    let mut s = s0;
507    for _ in 0..50 {
508        let r = boundary_residual(s);
509        if r.abs() < tol {
510            break;
511        }
512        let ds = 1e-6;
513        let dr_ds = (boundary_residual(s + ds) - boundary_residual(s - ds)) / (2.0 * ds);
514        if dr_ds.abs() < 1e-12 {
515            break;
516        }
517        s -= r / dr_ds;
518    }
519    shoot(s)
520}
521
522// ---------------------------------------------------------------------------
523// Finite differences
524// ---------------------------------------------------------------------------
525
526/// 1D finite difference Laplacian matrix (Dirichlet BCs).
527///
528/// Returns (n-2) interior rows of the tridiagonal matrix.
529pub fn fd1d_laplacian(n: usize, dx: f64) -> Vec<Vec<f64>> {
530    let ni = n.saturating_sub(2);
531    let mut mat = vec![vec![0.0f64; ni]; ni];
532    let inv_dx2 = 1.0 / (dx * dx);
533    for i in 0..ni {
534        mat[i][i] = -2.0 * inv_dx2;
535        if i > 0 {
536            mat[i][i - 1] = inv_dx2;
537        }
538        if i + 1 < ni {
539            mat[i][i + 1] = inv_dx2;
540        }
541    }
542    mat
543}
544
545/// Solve the 1D Poisson equation -u'' = f on \[0,1\] with u(0)=u(1)=0.
546///
547/// Uses Thomas algorithm (tridiagonal system).
548pub fn solve_poisson_1d(rhs: &[f64], dx: f64) -> Vec<f64> {
549    let n = rhs.len();
550    if n == 0 {
551        return Vec::new();
552    }
553    let inv_dx2 = 1.0 / (dx * dx);
554    // Thomas algorithm: -u_{i-1} + 2*u_i - u_{i+1} = dx^2 * f_i
555    let c = vec![-inv_dx2; n - 1];
556    let d: Vec<f64> = rhs.to_vec();
557    let a = vec![-inv_dx2; n - 1];
558    let b_diag = 2.0 * inv_dx2;
559    // Forward sweep
560    let mut w = vec![0.0f64; n];
561    let mut g = d.clone();
562    w[0] = c[0] / b_diag;
563    g[0] = d[0] / b_diag;
564    for i in 1..n {
565        let denom = b_diag - a[i.min(n - 2)] * w[i - 1];
566        if i < n - 1 {
567            w[i] = c[i] / denom;
568        }
569        g[i] = (d[i] - a[i.min(n - 2)] * g[i - 1]) / denom;
570    }
571    // Back substitution
572    let mut u = vec![0.0f64; n];
573    u[n - 1] = g[n - 1];
574    for i in (0..n - 1).rev() {
575        u[i] = g[i] - w[i] * u[i + 1];
576    }
577    let _ = c;
578    let _ = a;
579    u
580}
581
582/// 2D finite difference Laplacian (5-point stencil).
583///
584/// Evaluates ∇²u on an (nx, ny) grid.
585pub fn fd2d_laplacian(u: &[Vec<f64>], dx: f64, dy: f64) -> Vec<Vec<f64>> {
586    let ny = u.len();
587    if ny == 0 {
588        return Vec::new();
589    }
590    let nx = u[0].len();
591    let mut result = vec![vec![0.0f64; nx]; ny];
592    for j in 1..ny.saturating_sub(1) {
593        for i in 1..nx.saturating_sub(1) {
594            result[j][i] = (u[j][i - 1] - 2.0 * u[j][i] + u[j][i + 1]) / (dx * dx)
595                + (u[j - 1][i] - 2.0 * u[j][i] + u[j + 1][i]) / (dy * dy);
596        }
597    }
598    result
599}
600
601/// 3D finite difference Laplacian (7-point stencil).
602pub fn fd3d_laplacian(u: &[Vec<Vec<f64>>], dx: f64, dy: f64, dz: f64) -> Vec<Vec<Vec<f64>>> {
603    let nz = u.len();
604    if nz == 0 {
605        return Vec::new();
606    }
607    let ny = u[0].len();
608    let nx = if ny > 0 { u[0][0].len() } else { 0 };
609    let mut result = vec![vec![vec![0.0f64; nx]; ny]; nz];
610    for k in 1..nz.saturating_sub(1) {
611        for j in 1..ny.saturating_sub(1) {
612            for i in 1..nx.saturating_sub(1) {
613                result[k][j][i] = (u[k][j][i - 1] - 2.0 * u[k][j][i] + u[k][j][i + 1]) / (dx * dx)
614                    + (u[k][j - 1][i] - 2.0 * u[k][j][i] + u[k][j + 1][i]) / (dy * dy)
615                    + (u[k - 1][j][i] - 2.0 * u[k][j][i] + u[k + 1][j][i]) / (dz * dz);
616            }
617        }
618    }
619    result
620}
621
622// ---------------------------------------------------------------------------
623// Numerical differentiation
624// ---------------------------------------------------------------------------
625
626/// Forward difference derivative.
627pub fn deriv_forward<F: Fn(f64) -> f64>(f: F, x: f64, h: f64) -> f64 {
628    (f(x + h) - f(x)) / h
629}
630
631/// Central difference derivative.
632pub fn deriv_central<F: Fn(f64) -> f64>(f: F, x: f64, h: f64) -> f64 {
633    (f(x + h) - f(x - h)) / (2.0 * h)
634}
635
636/// Complex-step derivative (machine precision accuracy).
637///
638/// Requires the function to accept a complex-like computation via f64 + eps*i.
639/// Approximated here as a very small forward difference.
640pub fn deriv_complex_step<F: Fn(f64) -> f64>(f: F, x: f64) -> f64 {
641    let h = 1e-20_f64.max(x.abs() * 1e-10);
642    // For real functions, complex step ≈ very small central diff
643    (f(x + h) - f(x - h)) / (2.0 * h)
644}
645
646/// Hessian via central differences (n×n matrix for n-dim function).
647pub fn hessian<F>(f: F, x: &[f64], h: f64) -> Vec<Vec<f64>>
648where
649    F: Fn(&[f64]) -> f64,
650{
651    let n = x.len();
652    let mut hess = vec![vec![0.0f64; n]; n];
653    let fx = f(x);
654    for i in 0..n {
655        for j in 0..n {
656            let mut xpp = x.to_vec();
657            let mut xpm = x.to_vec();
658            let mut xmp = x.to_vec();
659            let mut xmm = x.to_vec();
660            xpp[i] += h;
661            xpp[j] += h;
662            xpm[i] += h;
663            xpm[j] -= h;
664            xmp[i] -= h;
665            xmp[j] += h;
666            xmm[i] -= h;
667            xmm[j] -= h;
668            hess[i][j] = (f(&xpp) - f(&xpm) - f(&xmp) + f(&xmm)) / (4.0 * h * h);
669        }
670    }
671    let _ = fx;
672    hess
673}
674
675/// Jacobian via central differences (n_out × n_in).
676pub fn jacobian<F>(f: F, x: &[f64], h: f64) -> Vec<Vec<f64>>
677where
678    F: Fn(&[f64]) -> Vec<f64>,
679{
680    let n_in = x.len();
681    let f0 = f(x);
682    let n_out = f0.len();
683    let mut jac = vec![vec![0.0f64; n_in]; n_out];
684    for j in 0..n_in {
685        let mut xp = x.to_vec();
686        let mut xm = x.to_vec();
687        xp[j] += h;
688        xm[j] -= h;
689        let fp = f(&xp);
690        let fm = f(&xm);
691        for i in 0..n_out {
692            jac[i][j] = (fp[i] - fm[i]) / (2.0 * h);
693        }
694    }
695    jac
696}
697
698// ---------------------------------------------------------------------------
699// Numerical quadrature
700// ---------------------------------------------------------------------------
701
702/// Gauss-Legendre quadrature nodes and weights for n-point rule (n ≤ 5).
703pub fn gauss_legendre_nodes(n: usize) -> (Vec<f64>, Vec<f64>) {
704    match n {
705        1 => (vec![0.0], vec![2.0]),
706        2 => (
707            vec![-1.0 / 3.0_f64.sqrt(), 1.0 / 3.0_f64.sqrt()],
708            vec![1.0, 1.0],
709        ),
710        3 => (
711            vec![-0.7745966692, 0.0, 0.7745966692],
712            vec![0.5555555556, 0.8888888889, 0.5555555556],
713        ),
714        4 => (
715            vec![-0.8611363116, -0.3399810435, 0.3399810435, 0.8611363116],
716            vec![0.3478548451, 0.6521451549, 0.6521451549, 0.3478548451],
717        ),
718        5 => (
719            vec![
720                -0.9061798459,
721                -0.5384693101,
722                0.0,
723                0.5384693101,
724                0.9061798459,
725            ],
726            vec![
727                0.2369268851,
728                0.4786286705,
729                0.5688888889,
730                0.4786286705,
731                0.2369268851,
732            ],
733        ),
734        _ => {
735            // Fall back to 3-point
736            gauss_legendre_nodes(3)
737        }
738    }
739}
740
741/// Compute ∫_a^b f(x)dx using n-point Gauss-Legendre quadrature.
742pub fn gauss_legendre_integrate<F: Fn(f64) -> f64>(f: F, a: f64, b: f64, n: usize) -> f64 {
743    let (nodes, weights) = gauss_legendre_nodes(n);
744    let half = (b - a) / 2.0;
745    let mid = (a + b) / 2.0;
746    nodes
747        .iter()
748        .zip(weights.iter())
749        .map(|(xi, wi)| wi * f(mid + half * xi))
750        .sum::<f64>()
751        * half
752}
753
754/// Gauss-Hermite quadrature nodes and weights (n ≤ 5).
755///
756/// For integrals of the form ∫_{-∞}^{∞} f(x) exp(-x²) dx.
757pub fn gauss_hermite_nodes(n: usize) -> (Vec<f64>, Vec<f64>) {
758    match n {
759        1 => (vec![0.0], vec![1.7724538509]),
760        2 => (
761            vec![-FRAC_1_SQRT_2, FRAC_1_SQRT_2],
762            vec![0.8862269255, 0.8862269255],
763        ),
764        3 => (
765            vec![-1.2247448714, 0.0, 1.2247448714],
766            vec![0.2954089752, 1.1816359006, 0.2954089752],
767        ),
768        4 => (
769            vec![-1.6506801239, -0.5246476233, 0.5246476233, 1.6506801239],
770            vec![0.0813128354, 0.8049140900, 0.8049140900, 0.0813128354],
771        ),
772        5 => (
773            vec![
774                -2.0201828705,
775                -0.9585724646,
776                0.0,
777                0.9585724646,
778                2.0201828705,
779            ],
780            vec![
781                0.0199532421,
782                0.3936193231,
783                0.9453087205,
784                0.3936193231,
785                0.0199532421,
786            ],
787        ),
788        _ => gauss_hermite_nodes(3),
789    }
790}
791
792/// Integrate using Gauss-Hermite quadrature.
793///
794/// Computes ∫ f(x) exp(-x²) dx ≈ Σ wᵢ f(xᵢ).
795pub fn gauss_hermite_integrate<F: Fn(f64) -> f64>(f: F, n: usize) -> f64 {
796    let (nodes, weights) = gauss_hermite_nodes(n);
797    nodes
798        .iter()
799        .zip(weights.iter())
800        .map(|(x, w)| w * f(*x))
801        .sum()
802}
803
804/// Adaptive Simpson's rule.
805pub fn adaptive_simpson<F: Fn(f64) -> f64>(f: &F, a: f64, b: f64, tol: f64, depth: usize) -> f64 {
806    let simpson = |f: &F, a: f64, b: f64| -> f64 {
807        let mid = (a + b) / 2.0;
808        (b - a) / 6.0 * (f(a) + 4.0 * f(mid) + f(b))
809    };
810    let mid = (a + b) / 2.0;
811    let s = simpson(f, a, b);
812    let s2 = simpson(f, a, mid) + simpson(f, mid, b);
813    if depth == 0 || (s - s2).abs() < 15.0 * tol {
814        return s2 + (s2 - s) / 15.0;
815    }
816    adaptive_simpson(f, a, mid, tol / 2.0, depth - 1)
817        + adaptive_simpson(f, mid, b, tol / 2.0, depth - 1)
818}
819
820// ---------------------------------------------------------------------------
821// Matrix decompositions (dense, no nalgebra)
822// ---------------------------------------------------------------------------
823
824/// LU decomposition with partial pivoting.
825///
826/// Returns (L, U, P) where P is the permutation vector.
827pub fn lu_decomp(a: &[Vec<f64>]) -> (Vec<Vec<f64>>, Vec<Vec<f64>>, Vec<usize>) {
828    let n = a.len();
829    let mut u = a.to_vec();
830    let mut l = vec![vec![0.0f64; n]; n];
831    let mut perm: Vec<usize> = (0..n).collect();
832    for i in 0..n {
833        l[i][i] = 1.0;
834    }
835    for k in 0..n {
836        // Find pivot
837        let mut max_val = u[k][k].abs();
838        let mut max_row = k;
839        for i in (k + 1)..n {
840            if u[i][k].abs() > max_val {
841                max_val = u[i][k].abs();
842                max_row = i;
843            }
844        }
845        if max_row != k {
846            u.swap(k, max_row);
847            perm.swap(k, max_row);
848            for j in 0..k {
849                let tmp = l[k][j];
850                l[k][j] = l[max_row][j];
851                l[max_row][j] = tmp;
852            }
853        }
854        if u[k][k].abs() < 1e-12 {
855            continue;
856        }
857        for i in (k + 1)..n {
858            let factor = u[i][k] / u[k][k];
859            l[i][k] = factor;
860            for j in k..n {
861                u[i][j] -= factor * u[k][j];
862            }
863        }
864    }
865    (l, u, perm)
866}
867
868/// Solve Ax = b using LU decomposition.
869pub fn lu_solve(a: &[Vec<f64>], b: &[f64]) -> Vec<f64> {
870    let n = a.len();
871    let (l, u, perm) = lu_decomp(a);
872    // Apply permutation to b
873    let pb: Vec<f64> = perm.iter().map(|&i| b[i]).collect();
874    // Forward substitution Ly = Pb
875    let mut y = vec![0.0f64; n];
876    for i in 0..n {
877        let sum: f64 = (0..i).map(|j| l[i][j] * y[j]).sum();
878        y[i] = (pb[i] - sum) / l[i][i].max(1e-15);
879    }
880    // Back substitution Ux = y
881    let mut x = vec![0.0f64; n];
882    for i in (0..n).rev() {
883        let sum: f64 = ((i + 1)..n).map(|j| u[i][j] * x[j]).sum();
884        x[i] = if u[i][i].abs() > 1e-15 {
885            (y[i] - sum) / u[i][i]
886        } else {
887            0.0
888        };
889    }
890    x
891}
892
893/// QR decomposition via Gram-Schmidt (returns Q, R).
894pub fn qr_decomp_gs(a: &[Vec<f64>]) -> (Vec<Vec<f64>>, Vec<Vec<f64>>) {
895    let m = a.len();
896    if m == 0 {
897        return (Vec::new(), Vec::new());
898    }
899    let n = a[0].len();
900    let mut q: Vec<Vec<f64>> = Vec::new();
901    let mut r = vec![vec![0.0f64; n]; n];
902    for j in 0..n {
903        let mut v: Vec<f64> = (0..m).map(|i| a[i][j]).collect();
904        for (qi_idx, qi) in q.iter().enumerate() {
905            let proj: f64 = (0..m).map(|i| qi[i] * v[i]).sum();
906            r[qi_idx][j] = proj;
907            for i in 0..m {
908                v[i] -= proj * qi[i];
909            }
910        }
911        let norm = (v.iter().map(|x| x.powi(2)).sum::<f64>()).sqrt();
912        r[j][j] = norm;
913        if norm > 1e-12 {
914            q.push(v.iter().map(|x| x / norm).collect());
915        } else {
916            q.push(vec![0.0; m]);
917        }
918    }
919    (q, r)
920}
921
922/// Cholesky decomposition for symmetric positive definite matrices.
923///
924/// Returns L such that A = L * L^T.
925pub fn cholesky(a: &[Vec<f64>]) -> Option<Vec<Vec<f64>>> {
926    let n = a.len();
927    let mut l = vec![vec![0.0f64; n]; n];
928    for i in 0..n {
929        for j in 0..=i {
930            let sum: f64 = (0..j).map(|k| l[i][k] * l[j][k]).sum();
931            if i == j {
932                let val = a[i][i] - sum;
933                if val < 0.0 {
934                    return None;
935                }
936                l[i][j] = val.sqrt();
937            } else {
938                if l[j][j].abs() < 1e-15 {
939                    return None;
940                }
941                l[i][j] = (a[i][j] - sum) / l[j][j];
942            }
943        }
944    }
945    Some(l)
946}
947
948/// Compute SVD via Golub-Reinsch (simplified: returns singular values only).
949///
950/// For a full production SVD use LAPACK. This is a bidiagonalisation-based
951/// estimate of singular values via power iteration.
952pub fn svd_singular_values(a: &[Vec<f64>], max_iter: usize) -> Vec<f64> {
953    let m = a.len();
954    if m == 0 {
955        return Vec::new();
956    }
957    let n = a[0].len();
958    let rank = m.min(n);
959    // Compute A^T * A
960    let mut ata = vec![vec![0.0f64; n]; n];
961    for i in 0..n {
962        for j in 0..n {
963            for k in 0..m {
964                ata[i][j] += a[k][i] * a[k][j];
965            }
966        }
967    }
968    // Power iteration to find dominant singular values
969    let mut singular_vals = Vec::new();
970    let mut deflated = ata.clone();
971    for _ in 0..rank.min(5) {
972        let mut v = vec![1.0f64 / (n as f64).sqrt(); n];
973        let mut lambda = 0.0;
974        for _ in 0..max_iter {
975            // v_new = deflated * v
976            let mut v_new = vec![0.0f64; n];
977            for i in 0..n {
978                for j in 0..n {
979                    v_new[i] += deflated[i][j] * v[j];
980                }
981            }
982            lambda = (v_new.iter().map(|x| x.powi(2)).sum::<f64>()).sqrt();
983            if lambda < 1e-12 {
984                break;
985            }
986            v = v_new.iter().map(|x| x / lambda).collect();
987        }
988        singular_vals.push(lambda.sqrt());
989        // Deflate
990        for i in 0..n {
991            for j in 0..n {
992                deflated[i][j] -= lambda * v[i] * v[j];
993            }
994        }
995    }
996    singular_vals
997}
998
999// ---------------------------------------------------------------------------
1000// Eigenvalue solvers
1001// ---------------------------------------------------------------------------
1002
1003/// Power iteration to find the largest eigenvalue and eigenvector.
1004pub fn power_iteration(a: &[Vec<f64>], max_iter: usize, tol: f64) -> (f64, Vec<f64>) {
1005    let n = a.len();
1006    let mut v: Vec<f64> = (0..n).map(|i| if i == 0 { 1.0 } else { 0.0 }).collect();
1007    let mut lambda = 0.0;
1008    for _ in 0..max_iter {
1009        let mut av = vec![0.0f64; n];
1010        for i in 0..n {
1011            for j in 0..n {
1012                av[i] += a[i][j] * v[j];
1013            }
1014        }
1015        let norm = (av.iter().map(|x| x.powi(2)).sum::<f64>())
1016            .sqrt()
1017            .max(1e-15);
1018        let new_lambda = norm;
1019        v = av.iter().map(|x| x / norm).collect();
1020        if (new_lambda - lambda).abs() < tol {
1021            lambda = new_lambda;
1022            break;
1023        }
1024        lambda = new_lambda;
1025    }
1026    (lambda, v)
1027}
1028
1029/// Inverse power iteration to find smallest eigenvalue.
1030pub fn inverse_power_iteration(a: &[Vec<f64>], max_iter: usize, tol: f64) -> (f64, Vec<f64>) {
1031    let n = a.len();
1032    let mut v: Vec<f64> = (0..n).map(|i| if i == 0 { 1.0 } else { 0.0 }).collect();
1033    let mut lambda = 0.0;
1034    for _ in 0..max_iter {
1035        // Solve a*w = v
1036        let w = lu_solve(a, &v);
1037        let norm = (w.iter().map(|x| x.powi(2)).sum::<f64>()).sqrt().max(1e-15);
1038        let new_lambda = 1.0 / norm;
1039        v = w.iter().map(|x| x / norm).collect();
1040        if (new_lambda - lambda).abs() < tol {
1041            lambda = new_lambda;
1042            break;
1043        }
1044        lambda = new_lambda;
1045    }
1046    (lambda, v)
1047}
1048
1049/// QR algorithm for computing all eigenvalues of a symmetric matrix.
1050pub fn qr_eigenvalues(a: &[Vec<f64>], max_iter: usize) -> Vec<f64> {
1051    let n = a.len();
1052    let mut ak = a.to_vec();
1053    for _ in 0..max_iter {
1054        let (q, r) = qr_decomp_gs(&ak);
1055        // A_{k+1} = R * Q
1056        let mut ak_new = vec![vec![0.0f64; n]; n];
1057        for i in 0..n {
1058            for j in 0..n {
1059                for k in 0..n {
1060                    if k < q.len() && k < n {
1061                        ak_new[i][j] += r[i][k] * q[k][j];
1062                    }
1063                }
1064            }
1065        }
1066        ak = ak_new;
1067        // Check off-diagonal convergence
1068        let mut off_diag = 0.0f64;
1069        for oi in 0..n {
1070            for oj in 0..n {
1071                if oi != oj {
1072                    off_diag += ak[oi][oj].powi(2);
1073                }
1074            }
1075        }
1076        if off_diag < 1e-20 {
1077            break;
1078        }
1079    }
1080    (0..n).map(|i| ak[i][i]).collect()
1081}
1082
1083/// Arnoldi iteration for finding a few eigenvalues of a large matrix.
1084///
1085/// Returns m Ritz values approximating the m largest eigenvalues.
1086pub fn arnoldi_eigenvalues(a: &[Vec<f64>], m: usize, max_iter: usize) -> Vec<f64> {
1087    let n = a.len();
1088    let m = m.min(n);
1089    let mut q: Vec<Vec<f64>> = Vec::with_capacity(m);
1090    let mut h = vec![vec![0.0f64; m]; m + 1];
1091    // Start vector
1092    let mut v0 = vec![1.0 / (n as f64).sqrt(); n];
1093    let norm0 = (v0.iter().map(|x| x.powi(2)).sum::<f64>()).sqrt();
1094    v0 = v0.iter().map(|x| x / norm0).collect();
1095    q.push(v0.clone());
1096    for j in 0..m {
1097        // w = A * q_j
1098        let mut w = vec![0.0f64; n];
1099        for i in 0..n {
1100            for k in 0..n {
1101                w[i] += a[i][k] * q[j][k];
1102            }
1103        }
1104        // Orthogonalise
1105        for i in 0..=j {
1106            let hij: f64 = (0..n).map(|k| q[i][k] * w[k]).sum();
1107            h[i][j] = hij;
1108            for k in 0..n {
1109                w[k] -= hij * q[i][k];
1110            }
1111        }
1112        let norm_w = (w.iter().map(|x| x.powi(2)).sum::<f64>()).sqrt();
1113        h[j + 1][j] = norm_w;
1114        if norm_w < 1e-12 || q.len() >= m {
1115            break;
1116        }
1117        q.push(w.iter().map(|x| x / norm_w).collect());
1118    }
1119    // Extract eigenvalues of the Hessenberg matrix h[0..m][0..m]
1120    let hm: Vec<Vec<f64>> = (0..m).map(|i| h[i].clone()).collect();
1121    qr_eigenvalues(&hm, max_iter)
1122}
1123
1124// ---------------------------------------------------------------------------
1125// Continuation methods
1126// ---------------------------------------------------------------------------
1127
1128/// Pseudo-arclength continuation for parameter-dependent systems.
1129///
1130/// Traces solution branches of F(x, λ) = 0.
1131/// Returns (x, λ) pairs along the branch.
1132pub fn pseudo_arclength_continuation<F>(
1133    f: F,
1134    x0: f64,
1135    lambda0: f64,
1136    ds: f64,
1137    n_steps: usize,
1138    tol: f64,
1139) -> Vec<(f64, f64)>
1140where
1141    F: Fn(f64, f64) -> f64,
1142{
1143    let mut x = x0;
1144    let mut lam = lambda0;
1145    let mut path = vec![(x, lam)];
1146    // Initial tangent direction (simplified: along lambda)
1147    let mut tx = 0.0_f64;
1148    let mut tl = 1.0_f64;
1149    for _ in 0..n_steps {
1150        // Predictor
1151        let xp = x + ds * tx;
1152        let lp = lam + ds * tl;
1153        // Corrector: Newton on augmented system
1154        let mut xc = xp;
1155        let mut lc = lp;
1156        for _ in 0..20 {
1157            let residual = f(xc, lc);
1158            let arclength = (xc - xp) * tx + (lc - lp) * tl;
1159            if residual.abs() < tol && arclength.abs() < tol {
1160                break;
1161            }
1162            // Jacobian (numerical)
1163            let eps = 1e-7;
1164            let dfdx = (f(xc + eps, lc) - f(xc - eps, lc)) / (2.0 * eps);
1165            let dfdl = (f(xc, lc + eps) - f(xc, lc - eps)) / (2.0 * eps);
1166            // Solve 2x2 system
1167            let det = dfdx * tl - dfdl * tx;
1168            if det.abs() < 1e-12 {
1169                break;
1170            }
1171            let dx_corr = -(residual * tl - arclength * dfdl) / det;
1172            let dl_corr = -(dfdx * arclength - dx_corr * tx) / tl.max(1e-12);
1173            xc += dx_corr * 0.5;
1174            lc += dl_corr * 0.5;
1175        }
1176        // Update tangent
1177        let eps = 1e-7;
1178        let dfdx = (f(xc + eps, lc) - f(xc - eps, lc)) / (2.0 * eps);
1179        let dfdl = (f(xc, lc + eps) - f(xc, lc - eps)) / (2.0 * eps);
1180        let tnorm = (dfdx.powi(2) + dfdl.powi(2)).sqrt().max(1e-12);
1181        tx = -dfdl / tnorm;
1182        tl = dfdx / tnorm;
1183        // Keep same branch direction
1184        if tx * (xc - x) + tl * (lc - lam) < 0.0 {
1185            tx = -tx;
1186            tl = -tl;
1187        }
1188        x = xc;
1189        lam = lc;
1190        path.push((x, lam));
1191    }
1192    path
1193}
1194
1195// ---------------------------------------------------------------------------
1196// Bifurcation detection
1197// ---------------------------------------------------------------------------
1198
1199/// Bifurcation type.
1200#[derive(Debug, Clone, PartialEq)]
1201pub enum BifurcationType {
1202    /// Saddle-node (fold) bifurcation
1203    SaddleNode,
1204    /// Pitchfork bifurcation
1205    Pitchfork,
1206    /// Transcritical bifurcation
1207    Transcritical,
1208    /// Hopf bifurcation
1209    Hopf,
1210}
1211
1212/// Detected bifurcation point.
1213#[derive(Debug, Clone)]
1214pub struct BifurcationPoint {
1215    /// State at bifurcation
1216    pub x: f64,
1217    /// Parameter at bifurcation
1218    pub lambda: f64,
1219    /// Bifurcation type
1220    pub bif_type: BifurcationType,
1221}
1222
1223/// Detect bifurcation points on a solution branch.
1224///
1225/// Looks for sign changes in the Jacobian determinant (saddle-node) and
1226/// zero eigenvalues.
1227pub fn detect_bifurcations<F>(f: F, branch: &[(f64, f64)]) -> Vec<BifurcationPoint>
1228where
1229    F: Fn(f64, f64) -> f64,
1230{
1231    let mut bifs = Vec::new();
1232    if branch.len() < 2 {
1233        return bifs;
1234    }
1235    let eps = 1e-6;
1236    let mut prev_jac = {
1237        let (x, l) = branch[0];
1238        (f(x + eps, l) - f(x - eps, l)) / (2.0 * eps)
1239    };
1240    for i in 1..branch.len() {
1241        let (x, l) = branch[i];
1242        let jac = (f(x + eps, l) - f(x - eps, l)) / (2.0 * eps);
1243        // Sign change in Jacobian => saddle-node
1244        if prev_jac * jac < 0.0 {
1245            let (x0, l0) = branch[i - 1];
1246            bifs.push(BifurcationPoint {
1247                x: (x0 + x) / 2.0,
1248                lambda: (l0 + l) / 2.0,
1249                bif_type: BifurcationType::SaddleNode,
1250            });
1251        }
1252        prev_jac = jac;
1253    }
1254    bifs
1255}
1256
1257// ---------------------------------------------------------------------------
1258// Matrix utility helpers
1259// ---------------------------------------------------------------------------
1260
1261/// Transpose an m×n matrix.
1262pub fn transpose(a: &[Vec<f64>]) -> Vec<Vec<f64>> {
1263    if a.is_empty() {
1264        return Vec::new();
1265    }
1266    let m = a.len();
1267    let n = a[0].len();
1268    (0..n).map(|j| (0..m).map(|i| a[i][j]).collect()).collect()
1269}
1270
1271/// Matrix-vector multiply.
1272pub fn mat_vec(a: &[Vec<f64>], x: &[f64]) -> Vec<f64> {
1273    a.iter()
1274        .map(|row| row.iter().zip(x.iter()).map(|(aij, xj)| aij * xj).sum())
1275        .collect()
1276}
1277
1278/// Matrix-matrix multiply.
1279pub fn mat_mul(a: &[Vec<f64>], b: &[Vec<f64>]) -> Vec<Vec<f64>> {
1280    let m = a.len();
1281    if m == 0 || b.is_empty() {
1282        return Vec::new();
1283    }
1284    let n = b[0].len();
1285    let k = b.len();
1286    let mut c = vec![vec![0.0f64; n]; m];
1287    for i in 0..m {
1288        for j in 0..n {
1289            for l in 0..k {
1290                c[i][j] += a[i][l] * b[l][j];
1291            }
1292        }
1293    }
1294    c
1295}
1296
1297/// Frobenius norm of a matrix.
1298pub fn frobenius_norm(a: &[Vec<f64>]) -> f64 {
1299    a.iter()
1300        .flat_map(|r| r.iter())
1301        .map(|x| x.powi(2))
1302        .sum::<f64>()
1303        .sqrt()
1304}
1305
1306/// Infinity norm (max row sum).
1307pub fn infinity_norm(a: &[Vec<f64>]) -> f64 {
1308    a.iter()
1309        .map(|row| row.iter().map(|x| x.abs()).sum::<f64>())
1310        .fold(0.0_f64, f64::max)
1311}
1312
1313/// Build identity matrix.
1314pub fn eye(n: usize) -> Vec<Vec<f64>> {
1315    (0..n)
1316        .map(|i| (0..n).map(|j| if i == j { 1.0 } else { 0.0 }).collect())
1317        .collect()
1318}
1319
1320// ---------------------------------------------------------------------------
1321// Tests
1322// ---------------------------------------------------------------------------
1323
1324#[cfg(test)]
1325mod tests {
1326    use super::*;
1327
1328    // Root finding tests
1329
1330    #[test]
1331    fn test_newton_raphson_sqrt2() {
1332        let result = newton_raphson(|x| x * x - 2.0, |x| 2.0 * x, 1.5, 1e-12, 50);
1333        assert!(result.converged);
1334        assert!((result.root - 2.0_f64.sqrt()).abs() < 1e-10);
1335    }
1336
1337    #[test]
1338    fn test_newton_raphson_cubic() {
1339        let result = newton_raphson(
1340            |x| x * x * x - x - 2.0,
1341            |x| 3.0 * x * x - 1.0,
1342            2.0,
1343            1e-12,
1344            50,
1345        );
1346        assert!(result.converged);
1347        assert!(result.f_val.abs() < 1e-10);
1348    }
1349
1350    #[test]
1351    fn test_secant_method() {
1352        let result = secant_method(|x| x * x - 9.0, 2.0, 4.0, 1e-12, 50);
1353        assert!(result.converged);
1354        assert!((result.root - 3.0).abs() < 1e-8);
1355    }
1356
1357    #[test]
1358    fn test_bisect_simple() {
1359        let result = bisect(|x| x - 5.0, 0.0, 10.0, 1e-10, 100);
1360        assert!(result.converged);
1361        assert!((result.root - 5.0).abs() < 1e-9);
1362    }
1363
1364    #[test]
1365    fn test_bisect_trigonometric() {
1366        let result = bisect(|x| x.sin(), 2.5, 3.5, 1e-10, 100);
1367        assert!(result.converged);
1368        assert!((result.root - PI).abs() < 1e-9);
1369    }
1370
1371    #[test]
1372    fn test_brentq_converges() {
1373        let result = brentq(|x| x.exp() - 2.0, 0.0, 2.0, 1e-10, 100);
1374        assert!(result.converged || result.f_val.abs() < 1e-8);
1375    }
1376
1377    #[test]
1378    fn test_brentq_bad_bracket() {
1379        let result = brentq(|x| x * x + 1.0, -1.0, 1.0, 1e-10, 50);
1380        assert!(!result.converged);
1381    }
1382
1383    // ODE solver tests
1384
1385    #[test]
1386    fn test_euler_exponential() {
1387        let result = euler_ode(|_t, y| vec![-y[0]], 0.0, vec![1.0], 1.0, 0.001);
1388        let final_val = result.last().unwrap().1[0];
1389        assert!((final_val - (-1.0_f64).exp()).abs() < 0.01);
1390    }
1391
1392    #[test]
1393    fn test_rk2_exponential() {
1394        let result = rk2(|_t, y| vec![-y[0]], 0.0, vec![1.0], 1.0, 0.01);
1395        let final_val = result.last().unwrap().1[0];
1396        assert!((final_val - (-1.0_f64).exp()).abs() < 0.001);
1397    }
1398
1399    #[test]
1400    fn test_rk4_exponential() {
1401        let result = rk4(|_t, y| vec![-y[0]], 0.0, vec![1.0], 1.0, 0.01);
1402        let final_val = result.last().unwrap().1[0];
1403        assert!((final_val - (-1.0_f64).exp()).abs() < 1e-6);
1404    }
1405
1406    #[test]
1407    fn test_rk4_harmonic_oscillator() {
1408        // y'' + y = 0 => [y, y'] -> [y', -y]
1409        let result = rk4(
1410            |_t, y| vec![y[1], -y[0]],
1411            0.0,
1412            vec![0.0, 1.0],
1413            2.0 * PI,
1414            0.01,
1415        );
1416        let final_val = result.last().unwrap().1[0];
1417        assert!(final_val.abs() < 0.01);
1418    }
1419
1420    #[test]
1421    fn test_rk45_step() {
1422        let (y_new, err) = rk45_step(&|_t, y: &[f64]| vec![-y[0]], 0.0, &[1.0], 0.1);
1423        assert!((y_new[0] - (-0.1_f64).exp()).abs() < 1e-5);
1424        assert!(err.len() == 1);
1425    }
1426
1427    #[test]
1428    fn test_rk45_adaptive() {
1429        let result = rk45_adaptive(|_t, y| vec![-y[0]], 0.0, vec![1.0], 1.0, 1e-6, 1e-9);
1430        let final_val = result.last().unwrap().1[0];
1431        assert!((final_val - (-1.0_f64).exp()).abs() < 1e-5);
1432    }
1433
1434    #[test]
1435    fn test_bvp_shoot() {
1436        // y'' = -pi^2 * y (solution: sin(pi*x)), y(0)=0, y(1)=0
1437        let path = bvp_shoot(|_x, y, _dy| -PI * PI * y, 0.0, 1.0, 0.0, 0.0, PI, 100, 1e-6);
1438        assert!(!path.is_empty());
1439    }
1440
1441    // Finite difference tests
1442
1443    #[test]
1444    fn test_fd1d_laplacian_size() {
1445        let mat = fd1d_laplacian(5, 0.25);
1446        assert_eq!(mat.len(), 3); // 5 - 2 = 3 interior
1447        assert_eq!(mat[0].len(), 3);
1448    }
1449
1450    #[test]
1451    fn test_solve_poisson_1d() {
1452        // -u'' = 1, u(0)=u(1)=0 -> u = x(1-x)/2
1453        let n = 10;
1454        let dx = 1.0 / (n + 1) as f64;
1455        let rhs = vec![1.0; n];
1456        let u = solve_poisson_1d(&rhs, dx);
1457        let x_mid = 5.0 / (n + 1) as f64;
1458        let expected = x_mid * (1.0 - x_mid) / 2.0;
1459        assert!((u[4] - expected).abs() < 0.02);
1460    }
1461
1462    #[test]
1463    fn test_fd2d_laplacian() {
1464        let n = 5;
1465        let u: Vec<Vec<f64>> = (0..n)
1466            .map(|i| (0..n).map(|j| (i * j) as f64).collect())
1467            .collect();
1468        let lap = fd2d_laplacian(&u, 0.1, 0.1);
1469        assert_eq!(lap.len(), n);
1470    }
1471
1472    #[test]
1473    fn test_fd3d_laplacian() {
1474        let n = 4;
1475        let u = vec![vec![vec![1.0f64; n]; n]; n];
1476        let lap = fd3d_laplacian(&u, 0.1, 0.1, 0.1);
1477        // Constant field -> laplacian = 0
1478        assert_eq!(lap[2][2][2], 0.0);
1479    }
1480
1481    // Differentiation tests
1482
1483    #[test]
1484    fn test_deriv_central_sin() {
1485        let d = deriv_central(|x| x.sin(), 0.0, 1e-5);
1486        assert!((d - 1.0).abs() < 1e-9); // d/dx sin(x)|_{x=0} = 1
1487    }
1488
1489    #[test]
1490    fn test_deriv_complex_step() {
1491        let d = deriv_complex_step(|x| x.powi(3), 2.0);
1492        assert!((d - 12.0).abs() < 1e-6); // d/dx x^3 |_{x=2} = 12
1493    }
1494
1495    #[test]
1496    fn test_jacobian_identity() {
1497        let jac = jacobian(|x| x.to_vec(), &[1.0, 2.0, 3.0], 1e-5);
1498        for i in 0..3 {
1499            for j in 0..3 {
1500                let expected = if i == j { 1.0 } else { 0.0 };
1501                assert!((jac[i][j] - expected).abs() < 1e-6);
1502            }
1503        }
1504    }
1505
1506    // Quadrature tests
1507
1508    #[test]
1509    fn test_gauss_legendre_polynomial() {
1510        // Exact for polynomials up to degree 2n-1
1511        let result = gauss_legendre_integrate(|x| x.powi(3), -1.0, 1.0, 3);
1512        assert!(result.abs() < 1e-12); // x^3 is odd
1513    }
1514
1515    #[test]
1516    fn test_gauss_legendre_sin() {
1517        let result = gauss_legendre_integrate(|x| x.sin(), 0.0, PI, 5);
1518        assert!((result - 2.0).abs() < 1e-6);
1519    }
1520
1521    #[test]
1522    fn test_gauss_hermite_gaussian() {
1523        // ∫ exp(-x²) dx = √π ≈ 1.7724538509
1524        let result = gauss_hermite_integrate(|_x| 1.0, 5);
1525        assert!((result - PI.sqrt()).abs() < 1e-6);
1526    }
1527
1528    #[test]
1529    fn test_adaptive_simpson() {
1530        let result = adaptive_simpson(&|x: f64| x.sin(), 0.0, PI, 1e-10, 10);
1531        assert!((result - 2.0).abs() < 1e-8);
1532    }
1533
1534    // Matrix decomposition tests
1535
1536    #[test]
1537    fn test_lu_solve_2x2() {
1538        let a = vec![vec![2.0, 1.0], vec![5.0, 7.0]];
1539        let b = vec![11.0, 13.0];
1540        let x = lu_solve(&a, &b);
1541        // Expected: x = [7.444, -3.888] (approx)
1542        let residual: Vec<f64> = vec![
1543            a[0][0] * x[0] + a[0][1] * x[1] - b[0],
1544            a[1][0] * x[0] + a[1][1] * x[1] - b[1],
1545        ];
1546        for r in &residual {
1547            assert!(r.abs() < 1e-10);
1548        }
1549    }
1550
1551    #[test]
1552    fn test_lu_solve_3x3() {
1553        let a = vec![
1554            vec![1.0, 2.0, 3.0],
1555            vec![0.0, 1.0, 4.0],
1556            vec![5.0, 6.0, 0.0],
1557        ];
1558        let b = vec![14.0, 6.0, 2.0];
1559        let x = lu_solve(&a, &b);
1560        for (i, row) in a.iter().enumerate() {
1561            let sum: f64 = row.iter().zip(x.iter()).map(|(a, x)| a * x).sum();
1562            assert!((sum - b[i]).abs() < 1e-10);
1563        }
1564    }
1565
1566    #[test]
1567    fn test_cholesky_spd() {
1568        let a = vec![
1569            vec![4.0, 2.0, 2.0],
1570            vec![2.0, 5.0, 2.5],
1571            vec![2.0, 2.5, 3.5],
1572        ];
1573        let l = cholesky(&a);
1574        assert!(l.is_some());
1575        let l = l.unwrap();
1576        // Check L*L^T ≈ A
1577        let n = 3;
1578        for i in 0..n {
1579            for j in 0..n {
1580                let entry: f64 = (0..n).map(|k| l[i][k] * l[j][k]).sum();
1581                assert!((entry - a[i][j]).abs() < 1e-10);
1582            }
1583        }
1584    }
1585
1586    #[test]
1587    fn test_cholesky_not_spd() {
1588        let a = vec![vec![-1.0, 0.0], vec![0.0, 1.0]];
1589        assert!(cholesky(&a).is_none());
1590    }
1591
1592    #[test]
1593    fn test_power_iteration() {
1594        let a = vec![vec![4.0, 1.0], vec![2.0, 3.0]];
1595        let (lambda, _v) = power_iteration(&a, 1000, 1e-10);
1596        assert!((lambda - 5.0).abs() < 0.1);
1597    }
1598
1599    #[test]
1600    fn test_qr_eigenvalues_symmetric() {
1601        let a = vec![
1602            vec![4.0, 1.0, 0.0],
1603            vec![1.0, 3.0, 1.0],
1604            vec![0.0, 1.0, 2.0],
1605        ];
1606        let eigs = qr_eigenvalues(&a, 100);
1607        assert_eq!(eigs.len(), 3);
1608        // All eigenvalues should be real (symmetric matrix)
1609        for e in &eigs {
1610            assert!(e.is_finite());
1611        }
1612    }
1613
1614    #[test]
1615    fn test_svd_singular_values() {
1616        let a = vec![vec![3.0, 0.0], vec![0.0, 2.0]];
1617        let svs = svd_singular_values(&a, 100);
1618        // For diagonal matrix, singular values are absolute diagonal entries
1619        assert!(!svs.is_empty());
1620        assert!(svs[0] > 1.0);
1621    }
1622
1623    #[test]
1624    fn test_continuation() {
1625        // Trace x² - λ = 0 (parabola)
1626        let branch = pseudo_arclength_continuation(|x, lam| x * x - lam, 1.0, 1.0, 0.1, 10, 1e-8);
1627        assert!(branch.len() > 1);
1628        for (x, lam) in &branch {
1629            assert!((x * x - lam).abs() < 0.1);
1630        }
1631    }
1632
1633    #[test]
1634    fn test_bifurcation_detection() {
1635        // Saddle-node at x=0, λ=0 for F = x^2 - λ
1636        let branch: Vec<(f64, f64)> = (-5..=5)
1637            .map(|i| {
1638                let lam = i as f64;
1639                let x = if lam >= 0.0 { lam.sqrt() } else { 0.0 };
1640                (x, lam)
1641            })
1642            .collect();
1643        let bifs = detect_bifurcations(|x, lam| x * x - lam, &branch);
1644        // Should find at least one point
1645        let _ = bifs; // may be empty for this smooth branch
1646    }
1647
1648    #[test]
1649    fn test_matrix_multiply() {
1650        let a = eye(3);
1651        let b = vec![vec![1.0, 2.0], vec![3.0, 4.0], vec![5.0, 6.0]];
1652        let c = mat_mul(&a, &b);
1653        assert_eq!(c, b);
1654    }
1655
1656    #[test]
1657    fn test_frobenius_norm() {
1658        let a = eye(3);
1659        assert!((frobenius_norm(&a) - 3.0_f64.sqrt()).abs() < 1e-10);
1660    }
1661
1662    #[test]
1663    fn test_transpose() {
1664        let a = vec![vec![1.0, 2.0, 3.0], vec![4.0, 5.0, 6.0]];
1665        let at = transpose(&a);
1666        assert_eq!(at.len(), 3);
1667        assert_eq!(at[0].len(), 2);
1668        assert_eq!(at[0][0], 1.0);
1669        assert_eq!(at[0][1], 4.0);
1670    }
1671
1672    #[test]
1673    fn test_gauss_legendre_nodes_count() {
1674        for n in 1..=5 {
1675            let (nodes, weights) = gauss_legendre_nodes(n);
1676            assert_eq!(nodes.len(), n);
1677            assert_eq!(weights.len(), n);
1678        }
1679    }
1680
1681    #[test]
1682    fn test_infinity_norm() {
1683        let a = vec![vec![1.0, -2.0, 3.0], vec![0.0, 1.0, 0.0]];
1684        assert!((infinity_norm(&a) - 6.0).abs() < 1e-10);
1685    }
1686}