use std::f64::consts::PI;
#[derive(Clone, Copy, Debug)]
struct Complex {
re: f64,
im: f64,
}
impl Complex {
fn new(re: f64, im: f64) -> Self { Complex { re, im } }
fn add(&self, other: &Complex) -> Complex { Complex::new(self.re + other.re, self.im + other.im) }
fn mul(&self, other: &Complex) -> Complex {
Complex::new(self.re * other.re - self.im * other.im, self.re * other.im + self.im * other.re)
}
fn from_polar(r: f64, theta: f64) -> Complex { Complex::new(r * theta.cos(), r * theta.sin()) }
fn norm_sq(&self) -> f64 { self.re * self.re + self.im * self.im }
fn scale(&self, scalar: f64) -> Complex { Complex::new(self.re * scalar, self.im * scalar) }
}
struct LCG { seed: u64 }
impl LCG {
fn new(seed: u64) -> Self { LCG { seed } }
fn next_f64(&mut self) -> f64 {
self.seed = self.seed.wrapping_mul(6364136223846793005).wrapping_add(1442695040888963407);
(self.seed >> 11) as f64 / (1u64 << 53) as f64
}
}
#[derive(Clone)]
struct QIC3QubitState {
amplitudes: [Complex; 8],
}
impl QIC3QubitState {
fn new_normalized_uniform() -> Self {
let mut state = QIC3QubitState { amplitudes: [Complex::new(0.0, 0.0); 8] };
let norm_factor = 1.0 / (8.0_f64).sqrt();
for i in 0..8 {
state.amplitudes[i] = Complex::new(norm_factor, 0.0);
}
state
}
fn apply_noise(&mut self, noise_level: f64, prng: &mut LCG) {
for i in 0..8 {
let n_re = (prng.next_f64() - 0.5) * noise_level;
let n_im = (prng.next_f64() - 0.5) * noise_level;
self.amplitudes[i] = self.amplitudes[i].add(&Complex::new(n_re, n_im));
}
self.normalize();
}
fn normalize(&mut self) {
let mut total_prob = 0.0;
for c in &self.amplitudes { total_prob += c.norm_sq(); }
let norm = total_prob.sqrt();
for i in 0..8 { self.amplitudes[i] = self.amplitudes[i].scale(1.0 / norm); }
}
fn print_state(&self, label: &str) {
println!("\n--- {} ---", label);
let labels = ["|000>", "|001>", "|010>", "|011>", "|100>", "|101>", "|110>", "|111>"];
for i in 0..8 {
println!(" {}: [{:.3} + {:.3}i] (Prob: {:.2}%)",
labels[i], self.amplitudes[i].re, self.amplitudes[i].im, self.amplitudes[i].norm_sq() * 100.0);
}
}
}
fn is_state_forbidden_by_golden_chain(state_index: usize) -> bool {
matches!(state_index, 0 | 1 | 4)
}
fn apply_qic_bgate(state: &mut QIC3QubitState) {
println!("\n[!] Applying Localized 3-Qubit QIC B-Gate...");
let r_i = Complex::from_polar(1.0, -4.0 * PI / 5.0);
let r_tau = Complex::from_polar(1.0, 3.0 * PI / 5.0);
for i in 0..8 {
if is_state_forbidden_by_golden_chain(i) {
state.amplitudes[i] = Complex::new(0.0, 0.0);
} else {
if i % 2 == 0 {
state.amplitudes[i] = state.amplitudes[i].mul(&r_i);
} else {
state.amplitudes[i] = state.amplitudes[i].mul(&r_tau);
}
}
}
state.normalize();
}
fn main() {
println!("=== Kronova AetherNet: Quasicrystal Inflation Code (QIC) ===");
println!("Simulating 3-Qubit localized B-Gate distillation on the Golden Chain.\n");
let mut prng = LCG::new(1618); let mut quantum_register = QIC3QubitState::new_normalized_uniform();
quantum_register.print_state("1. Initial Raw Physical State (Uniform Superposition)");
let noise_intensity = 0.25;
println!("\n[!] Warning: High-intensity environmental decoherence detected.");
quantum_register.apply_noise(noise_intensity, &mut prng);
quantum_register.print_state("2. Corrupted Physical State");
println!("\n>>> Executing Algorithm: Enforcing Golden Chain constraints.");
println!(">>> Applying B_gate = R_I * P_local + R_tau * (I - P_local).");
apply_qic_bgate(&mut quantum_register);
quantum_register.print_state("3. Final Topologically Protected State");
println!("\n=== Simulation Complete ===");
println!("Conclusion: The QIC successfully projected the noisy physical register");
println!("into the protected Fibonacci subspace. The forbidden '00' states (000, 001, 100)");
println!("were mathematically filtered out, and the topological braiding phases were");
println!("safely acquired by the valid Golden Chain permutations.");
}