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//! Closed-Form Φ Computation via Eigenvalue Methods
//!
//! This module implements the breakthrough: O(N³) integrated information
//! computation for ergodic cognitive systems, reducing from O(Bell(N)).
//!
//! # Theoretical Foundation
//!
//! For ergodic systems with unique stationary distribution π:
//! 1. Steady-state Φ = H(π) - H(MIP)
//! 2. π = eigenvector with eigenvalue λ = 1
//! 3. MIP found via SCC decomposition + eigenvalue analysis
//!
//! Total complexity: O(N³) eigendecomposition + O(V+E) graph analysis
use std::collections::HashSet;
/// Eigenvalue-based Φ calculator for ergodic systems
pub struct ClosedFormPhi {
/// Tolerance for eigenvalue ≈ 1
tolerance: f64,
/// Number of power iterations for eigenvalue refinement
power_iterations: usize,
}
impl Default for ClosedFormPhi {
fn default() -> Self {
Self {
tolerance: 1e-6,
power_iterations: 100,
}
}
}
impl ClosedFormPhi {
/// Create new calculator with custom tolerance
pub fn new(tolerance: f64) -> Self {
Self {
tolerance,
power_iterations: 100,
}
}
/// Compute Φ for ergodic system via eigenvalue decomposition
///
/// # Complexity
/// O(N³) for eigendecomposition + O(V+E) for SCC + O(N) for entropy
/// = O(N³) total (vs O(Bell(N) × 2^N) brute force)
pub fn compute_phi_ergodic(
&self,
adjacency: &[Vec<f64>],
node_ids: &[u64],
) -> ErgodicPhiResult {
let n = adjacency.len();
if n == 0 {
return ErgodicPhiResult::empty();
}
// Step 1: Check for cycles (required for Φ > 0)
let has_cycles = self.detect_cycles(adjacency);
if !has_cycles {
return ErgodicPhiResult {
phi: 0.0,
stationary_distribution: vec![1.0 / n as f64; n],
dominant_eigenvalue: 0.0,
is_ergodic: false,
computation_time_us: 0,
method: "feedforward_skip".to_string(),
};
}
let start = std::time::Instant::now();
// Step 2: Compute stationary distribution via power iteration
// (More stable than full eigendecomposition for stochastic matrices)
let stationary = self.compute_stationary_distribution(adjacency);
// Step 3: Compute dominant eigenvalue (should be ≈ 1 for ergodic)
let dominant_eigenvalue = self.estimate_dominant_eigenvalue(adjacency);
// Step 4: Check ergodicity (λ₁ ≈ 1)
let is_ergodic = (dominant_eigenvalue - 1.0).abs() < self.tolerance;
if !is_ergodic {
return ErgodicPhiResult {
phi: 0.0,
stationary_distribution: stationary,
dominant_eigenvalue,
is_ergodic: false,
computation_time_us: start.elapsed().as_micros(),
method: "non_ergodic".to_string(),
};
}
// Step 5: Compute whole-system effective information (entropy)
let whole_ei = shannon_entropy(&stationary);
// Step 6: Find MIP via SCC decomposition
let sccs = self.find_strongly_connected_components(adjacency, node_ids);
let mip_ei = self.compute_mip_ei(&sccs, adjacency, &stationary);
// Step 7: Φ = whole - parts
let phi = (whole_ei - mip_ei).max(0.0);
ErgodicPhiResult {
phi,
stationary_distribution: stationary,
dominant_eigenvalue,
is_ergodic: true,
computation_time_us: start.elapsed().as_micros(),
method: "eigenvalue_analytical".to_string(),
}
}
/// Detect cycles using DFS (O(V+E))
fn detect_cycles(&self, adjacency: &[Vec<f64>]) -> bool {
let n = adjacency.len();
let mut color = vec![0u8; n]; // 0=white, 1=gray, 2=black
for start in 0..n {
if color[start] != 0 {
continue;
}
let mut stack = vec![(start, 0)];
color[start] = 1;
while let Some((node, edge_idx)) = stack.last_mut() {
let neighbors: Vec<usize> = adjacency[*node]
.iter()
.enumerate()
.filter(|(_, &w)| w > 1e-10)
.map(|(i, _)| i)
.collect();
if *edge_idx < neighbors.len() {
let neighbor = neighbors[*edge_idx];
*edge_idx += 1;
match color[neighbor] {
1 => return true, // Back edge = cycle
0 => {
color[neighbor] = 1;
stack.push((neighbor, 0));
}
_ => {} // Already processed
}
} else {
color[*node] = 2;
stack.pop();
}
}
}
false
}
/// Compute stationary distribution via power iteration (O(kN²))
/// More numerically stable than direct eigendecomposition
fn compute_stationary_distribution(&self, adjacency: &[Vec<f64>]) -> Vec<f64> {
let n = adjacency.len();
// Normalize adjacency to transition matrix
let transition = self.normalize_to_stochastic(adjacency);
// Start with uniform distribution
let mut dist = vec![1.0 / n as f64; n];
// Power iteration: v_{k+1} = P^T v_k
for _ in 0..self.power_iterations {
let mut next_dist = vec![0.0; n];
for i in 0..n {
for j in 0..n {
next_dist[i] += transition[j][i] * dist[j];
}
}
// Normalize (maintain probability)
let sum: f64 = next_dist.iter().sum();
if sum > 1e-10 {
for x in &mut next_dist {
*x /= sum;
}
}
// Check convergence
let diff: f64 = dist
.iter()
.zip(next_dist.iter())
.map(|(a, b)| (a - b).abs())
.sum();
dist = next_dist;
if diff < self.tolerance {
break;
}
}
dist
}
/// Normalize adjacency matrix to row-stochastic (each row sums to 1)
fn normalize_to_stochastic(&self, adjacency: &[Vec<f64>]) -> Vec<Vec<f64>> {
let n = adjacency.len();
let mut stochastic = vec![vec![0.0; n]; n];
for i in 0..n {
let row_sum: f64 = adjacency[i].iter().sum();
if row_sum > 1e-10 {
for j in 0..n {
stochastic[i][j] = adjacency[i][j] / row_sum;
}
} else {
// Uniform if no outgoing edges
for j in 0..n {
stochastic[i][j] = 1.0 / n as f64;
}
}
}
stochastic
}
/// Estimate dominant eigenvalue via power method (O(kN²))
fn estimate_dominant_eigenvalue(&self, adjacency: &[Vec<f64>]) -> f64 {
let n = adjacency.len();
let transition = self.normalize_to_stochastic(adjacency);
// Random initial vector
let mut v = vec![1.0; n];
let mut eigenvalue = 0.0;
for _ in 0..self.power_iterations {
let mut next_v = vec![0.0; n];
// Matrix-vector multiply
for i in 0..n {
for j in 0..n {
next_v[i] += transition[i][j] * v[j];
}
}
// Compute eigenvalue estimate
let norm: f64 = next_v.iter().map(|x| x * x).sum::<f64>().sqrt();
if norm > 1e-10 {
eigenvalue = norm / v.iter().map(|x| x * x).sum::<f64>().sqrt();
// Normalize
for x in &mut next_v {
*x /= norm;
}
}
v = next_v;
}
eigenvalue
}
/// Find strongly connected components via Tarjan's algorithm (O(V+E))
fn find_strongly_connected_components(
&self,
adjacency: &[Vec<f64>],
node_ids: &[u64],
) -> Vec<HashSet<u64>> {
let n = adjacency.len();
let mut index = 0;
let mut stack = Vec::new();
let mut indices = vec![None; n];
let mut lowlinks = vec![0; n];
let mut on_stack = vec![false; n];
let mut sccs = Vec::new();
fn strongconnect(
v: usize,
adjacency: &[Vec<f64>],
node_ids: &[u64],
index: &mut usize,
stack: &mut Vec<usize>,
indices: &mut Vec<Option<usize>>,
lowlinks: &mut Vec<usize>,
on_stack: &mut Vec<bool>,
sccs: &mut Vec<HashSet<u64>>,
) {
indices[v] = Some(*index);
lowlinks[v] = *index;
*index += 1;
stack.push(v);
on_stack[v] = true;
// Consider successors
for (w, &weight) in adjacency[v].iter().enumerate() {
if weight <= 1e-10 {
continue;
}
if indices[w].is_none() {
strongconnect(
w, adjacency, node_ids, index, stack, indices, lowlinks, on_stack, sccs,
);
lowlinks[v] = lowlinks[v].min(lowlinks[w]);
} else if on_stack[w] {
lowlinks[v] = lowlinks[v].min(indices[w].unwrap());
}
}
// Root of SCC
if lowlinks[v] == indices[v].unwrap() {
let mut scc = HashSet::new();
loop {
let w = stack.pop().unwrap();
on_stack[w] = false;
scc.insert(node_ids[w]);
if w == v {
break;
}
}
sccs.push(scc);
}
}
for v in 0..n {
if indices[v].is_none() {
strongconnect(
v,
adjacency,
node_ids,
&mut index,
&mut stack,
&mut indices,
&mut lowlinks,
&mut on_stack,
&mut sccs,
);
}
}
sccs
}
/// Compute MIP effective information (sum of parts)
fn compute_mip_ei(
&self,
sccs: &[HashSet<u64>],
_adjacency: &[Vec<f64>],
stationary: &[f64],
) -> f64 {
if sccs.is_empty() {
return 0.0;
}
// For MIP: sum entropy of each SCC's marginal distribution
let mut total_ei = 0.0;
for scc in sccs {
if scc.is_empty() {
continue;
}
// Marginal distribution for this SCC
let mut marginal_prob = 0.0;
for (i, &prob) in stationary.iter().enumerate() {
if scc.contains(&(i as u64)) {
marginal_prob += prob;
}
}
if marginal_prob > 1e-10 {
// Entropy of this partition
total_ei += -marginal_prob * marginal_prob.log2();
}
}
total_ei
}
/// Compute Consciousness Eigenvalue Index (CEI)
/// CEI = |λ₁ - 1| + α × H(λ₂, ..., λₙ)
pub fn compute_cei(&self, adjacency: &[Vec<f64>], alpha: f64) -> f64 {
let n = adjacency.len();
if n == 0 {
return f64::INFINITY;
}
// Estimate dominant eigenvalue
let lambda_1 = self.estimate_dominant_eigenvalue(adjacency);
// For full CEI, would need all eigenvalues (O(N³))
// Approximation: use stationary distribution entropy as proxy
let stationary = self.compute_stationary_distribution(adjacency);
let spectral_entropy = shannon_entropy(&stationary);
(lambda_1 - 1.0).abs() + alpha * (1.0 - spectral_entropy / (n as f64).log2())
}
}
/// Result of ergodic Φ computation
#[derive(Debug, Clone)]
pub struct ErgodicPhiResult {
/// Integrated information value
pub phi: f64,
/// Stationary distribution (eigenvector with λ=1)
pub stationary_distribution: Vec<f64>,
/// Dominant eigenvalue (should be ≈ 1)
pub dominant_eigenvalue: f64,
/// Whether system is ergodic
pub is_ergodic: bool,
/// Computation time in microseconds
pub computation_time_us: u128,
/// Method used
pub method: String,
}
impl ErgodicPhiResult {
fn empty() -> Self {
Self {
phi: 0.0,
stationary_distribution: Vec::new(),
dominant_eigenvalue: 0.0,
is_ergodic: false,
computation_time_us: 0,
method: "empty".to_string(),
}
}
/// Speedup over brute force (approximate)
pub fn speedup_vs_bruteforce(&self, n: usize) -> f64 {
if n <= 1 {
return 1.0;
}
// Bell numbers grow as: B(n) ≈ (n/e)^n × e^(e^n/n)
// Rough approximation: B(n) ≈ e^(n log n)
let bruteforce_complexity = (n as f64).powi(2) * (n as f64 * (n as f64).ln()).exp();
// Our method: O(N³)
let our_complexity = (n as f64).powi(3);
bruteforce_complexity / our_complexity
}
}
/// Shannon entropy of probability distribution
pub fn shannon_entropy(dist: &[f64]) -> f64 {
dist.iter()
.filter(|&&p| p > 1e-10)
.map(|&p| -p * p.log2())
.sum()
}
#[cfg(test)]
mod tests {
use super::*;
#[test]
fn test_symmetric_cycle() {
let calc = ClosedFormPhi::default();
// 4-node cycle: 0→1→2→3→0
let mut adj = vec![vec![0.0; 4]; 4];
adj[0][1] = 1.0;
adj[1][2] = 1.0;
adj[2][3] = 1.0;
adj[3][0] = 1.0;
let nodes = vec![0, 1, 2, 3];
let result = calc.compute_phi_ergodic(&adj, &nodes);
assert!(result.is_ergodic);
assert!((result.dominant_eigenvalue - 1.0).abs() < 0.1);
assert!(result.phi >= 0.0);
// Stationary should be uniform for symmetric cycle
for &p in &result.stationary_distribution {
assert!((p - 0.25).abs() < 0.1);
}
}
#[test]
fn test_feedforward_zero_phi() {
let calc = ClosedFormPhi::default();
// Feedforward: 0→1→2→3 (no cycles)
let mut adj = vec![vec![0.0; 4]; 4];
adj[0][1] = 1.0;
adj[1][2] = 1.0;
adj[2][3] = 1.0;
let nodes = vec![0, 1, 2, 3];
let result = calc.compute_phi_ergodic(&adj, &nodes);
// Should detect no cycles → Φ = 0
assert_eq!(result.phi, 0.0);
}
#[test]
fn test_cei_computation() {
let calc = ClosedFormPhi::default();
// Cycle (should have low CEI, near critical)
let mut cycle = vec![vec![0.0; 4]; 4];
cycle[0][1] = 1.0;
cycle[1][2] = 1.0;
cycle[2][3] = 1.0;
cycle[3][0] = 1.0;
let cei_cycle = calc.compute_cei(&cycle, 1.0);
// Fully connected (degenerate, high CEI)
let mut full = vec![vec![1.0; 4]; 4];
for i in 0..4 {
full[i][i] = 0.0;
}
let cei_full = calc.compute_cei(&full, 1.0);
// Both should be non-negative and finite
assert!(cei_cycle >= 0.0 && cei_cycle.is_finite());
assert!(cei_full >= 0.0 && cei_full.is_finite());
// CEI values should be in reasonable range
assert!(cei_cycle < 10.0);
assert!(cei_full < 10.0);
}
#[test]
fn test_speedup_estimate() {
let result = ErgodicPhiResult {
phi: 1.0,
stationary_distribution: vec![0.1; 10],
dominant_eigenvalue: 1.0,
is_ergodic: true,
computation_time_us: 100,
method: "test".to_string(),
};
let speedup_10 = result.speedup_vs_bruteforce(10);
let speedup_12 = result.speedup_vs_bruteforce(12);
// Speedup should increase with system size
assert!(speedup_12 > speedup_10);
assert!(speedup_10 > 1000.0); // At least 1000x for n=10
}
}