|
|
| import numpy as np |
| import matplotlib.pyplot as plt |
| from scipy.integrate import solve_ivp |
|
|
| |
| hbar = 1.0545718e-34 |
| G = 6.67430e-11 |
| m1, m2 = 1.0, 1.0 |
| d = 2.0 |
| base_freq = 440.0 |
| intent_coefficient = 0.7 |
|
|
| |
| tunneling_factor = 0.4 |
| quantum_states = np.array([1, -1]) |
| entanglement_strength = 0.85 |
| decoherence_factor = 0.02 |
|
|
| |
| num_agents = 3 |
| agent_positions = np.array([[-d, 0], [0, 0], [d, 0]]) |
| agent_velocities = np.array([[0, 0.5], [0, -0.5], [0, 0.3]]) |
|
|
| |
| y0 = np.concatenate([pos + vel for pos, vel in zip(agent_positions, agent_velocities)]) |
|
|
| |
| def quantum_harmonic_dynamics(t, y): |
| positions = y[::4] |
| velocities = y[1::4] |
|
|
| accelerations = np.zeros_like(positions) |
|
|
| for i in range(num_agents): |
| for j in range(i + 1, num_agents): |
| r_ij = positions[j] - positions[i] |
| dist = np.linalg.norm(r_ij) |
| if dist > 1e-6: |
| force = (G * m1 * m2 / dist**3) * r_ij |
| accelerations[i] += force / m1 |
| accelerations[j] -= force / m2 |
|
|
| |
| quantum_modifier = np.dot(quantum_states, np.sin(2 * np.pi * base_freq * t / 1000)) * intent_coefficient |
| tunneling_shift = tunneling_factor * np.exp(-np.linalg.norm(positions) / hbar) if np.random.rand() < tunneling_factor else 0 |
| entangled_correction = entanglement_strength * np.exp(-np.linalg.norm(positions) / hbar) |
| decoherence_adjustment = decoherence_factor * (1 - np.exp(-np.linalg.norm(positions) / hbar)) |
|
|
| harmonic_force = np.full_like(positions, quantum_modifier + entangled_correction + tunneling_shift - decoherence_adjustment) |
| accelerations += harmonic_force |
|
|
| return np.concatenate([velocities.flatten(), accelerations.flatten()]) |
|
|
| |
| t_span = (0, 100) |
| t_eval = np.linspace(t_span[0], t_span[1], 2500) |
| sol = solve_ivp(quantum_harmonic_dynamics, t_span, y0, t_eval=t_eval, method='RK45') |
|
|
| |
| positions = sol.y[::4] |
| velocities = sol.y[1::4] |
|
|
| |
| plt.figure(figsize=(10, 10)) |
| colors = ['b', 'r', 'g'] |
| for i in range(num_agents): |
| plt.plot(positions[i], velocities[i], label=f'AI Node {i+1} (Quantum Resonance)', linewidth=2, color=colors[i]) |
|
|
| plt.plot(0, 0, 'ko', label='Core Equilibrium') |
| plt.xlabel('X Position') |
| plt.ylabel('Y Position') |
| plt.title('Codette Quantum Harmonic AI Multi-Agent Synchronization') |
| plt.legend() |
| plt.axis('equal') |
| plt.grid(True) |
| plt.tight_layout() |
| plt.savefig("Codette_Quantum_Harmonic_Framework.png") |
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