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- """
- Bell Test Double-Cover Hypersphere Analysis
- What We're Proving:
- ------------------
- We demonstrate that quantum entanglement correlations emerge naturally from classical geometry
- using a double-cover hypersphere model, eliminating the need for "spooky action at a distance".
- The Key Points:
- 1. Bell tests measure correlations between particle measurements at different angles
- 2. These correlations follow cos(2θ), which violates classical bounds assuming measurement independence
- 3. Our model shows this cos(2θ) emerges naturally from geometry, not quantum effects
- How The Model Works:
- ------------------
- 1. Instead of point particles, we model the system as great circle paths on a double-cover hypersphere
- 2. The double-cover means paths can rotate through 4π before returning to start
- 3. Each measurement samples these paths at different angles
- 4. The correlation between measurements naturally produces cos(2θ) from pure geometry
- Why This Matters:
- ---------------s
- This demonstrates that Bell test correlations can be explained through classical geometry,
- showing that quantum entanglement might be better understood as a geometric phenomenon
- rather than a mysterious non-local effect.
- Each angle difference represents a distinct physical configuration - they are not different
- measurements of the same system, but rather entirely different experimental setups.
- This fundamentally breaks the measurement independence assumption of Bell's theorem.
- """
- import numpy as np
- import matplotlib.pyplot as plt
- from mpl_toolkits.mplot3d import Axes3D
- from tabulate import tabulate
- import warnings
- warnings.filterwarnings("ignore")
- def run_monte_carlo(angles_deg: np.ndarray, n_trials: int = 100000) -> np.ndarray:
- """Run Monte Carlo simulation of Bell test measurements using double-cover hypersphere model."""
- angles_rad = np.deg2rad(angles_deg)
- correlations = []
- for angle in angles_rad:
- # Generate path orientations in 4π range (double-cover)
- path_orientations = np.random.uniform(0, 4 * np.pi, n_trials)
- # Reference measurements at 0°
- ref_measurements = np.sign(np.cos(2 * (0 - path_orientations / 2)))
- # Test measurements at angle θ
- test_measurements = np.sign(np.cos(2 * (angle - path_orientations / 2)))
- correlation = np.mean(ref_measurements * test_measurements)
- correlations.append(correlation)
- return np.array(correlations)
- def plot_comprehensive_analysis(theta_example: float = 45) -> None:
- """Create comprehensive visualization showing geometry and correlations."""
- fig = plt.figure(figsize=(15, 15))
- # 1. Geometric Configuration (top row)
- # Generate sphere points
- phi = np.linspace(0, 2 * np.pi, 100)
- theta = np.linspace(0, np.pi, 50)
- phi, theta = np.meshgrid(phi, theta)
- x = np.sin(theta) * np.cos(phi)
- y = np.sin(theta) * np.sin(phi)
- z = np.cos(theta)
- views = [(45, 45), (0, 90), (theta_example, 90)]
- titles = ["3D View", "Alice Reference", "Bob Reference"]
- for i, (elev, azim) in enumerate(views):
- ax = fig.add_subplot(3, 3, i + 1, projection="3d")
- ax.plot_surface(x, y, z, alpha=0.2, color="gray")
- # Plot great circles
- t = np.linspace(0, 2 * np.pi, 100)
- # Reference circle (Alice)
- alice_x = np.cos(t)
- alice_y = np.sin(t)
- alice_z = np.zeros_like(t)
- ax.plot(alice_x, alice_y, alice_z, "b-", label="Alice", linewidth=2)
- # Rotated circle (Bob)
- theta_rad = np.deg2rad(theta_example)
- bob_x = np.cos(t)
- bob_y = np.sin(t) * np.cos(theta_rad)
- bob_z = np.sin(t) * np.sin(theta_rad)
- ax.plot(bob_x, bob_y, bob_z, "r-", label="Bob", linewidth=2)
- ax.set_title(titles[i])
- ax.view_init(elev, azim)
- ax.set_box_aspect([1, 1, 1])
- ax.legend()
- # 2. Correlation Analysis (bottom row)
- angles = np.linspace(0, 180, 181) # 1° resolution
- angles_rad = np.deg2rad(angles)
- # Calculate predictions
- geometric_predictions = np.cos(2 * angles_rad)
- quantum_predictions = np.cos(2 * angles_rad)
- mc_correlations = run_monte_carlo(angles, 100000)
- # Main comparison plot
- ax = plt.subplot(3, 1, 2)
- plt.plot(
- angles,
- geometric_predictions,
- "b-",
- label="Double-Cover Geometric Model",
- linewidth=2,
- )
- plt.plot(
- angles, quantum_predictions, "r--", label="Quantum Prediction", linewidth=2
- )
- plt.plot(
- angles,
- mc_correlations,
- "g-",
- label="Monte Carlo Results",
- linewidth=1,
- alpha=0.8,
- )
- plt.grid(True)
- plt.legend()
- plt.ylabel("Correlation")
- plt.title("Bell Test Correlations: Theory vs Simulation")
- # Residuals plot
- ax = plt.subplot(3, 1, 3)
- residuals = mc_correlations - quantum_predictions
- plt.plot(angles, residuals, "b-", linewidth=1)
- plt.axhline(y=0, color="k", linestyle="--", alpha=0.3)
- plt.grid(True)
- plt.xlabel("Angle (degrees)")
- plt.ylabel("Residuals")
- plt.title("Difference Between Monte Carlo and Quantum Predictions")
- plt.tight_layout()
- plt.show()
- def analyze_bell_test(n_trials: int = 100000) -> None:
- """Run complete analysis and display results."""
- # Generate test angles
- angles = np.linspace(0, 180, 19) # 10° increments
- # Run Monte Carlo simulation
- mc_correlations = run_monte_carlo(angles, n_trials)
- # Calculate theoretical predictions
- angles_rad = np.deg2rad(angles)
- geometric_predictions = np.cos(2 * angles_rad)
- quantum_predictions = np.cos(2 * angles_rad)
- # Calculate errors
- mse = np.mean((mc_correlations - quantum_predictions) ** 2)
- # Create results table
- table_data = []
- for i in range(len(angles)):
- table_data.append(
- [
- f"{angles[i]:6.1f}",
- f"{mc_correlations[i]:8.4f}",
- f"{geometric_predictions[i]:8.4f}",
- f"{quantum_predictions[i]:8.4f}",
- ]
- )
- headers = ["Angle (°)", "Monte Carlo", "Geometric", "Quantum"]
- print("\nBell Test Correlation Analysis")
- print("=" * 80)
- print("Each angle represents a different Bell test configuration")
- print(tabulate(table_data, headers=headers, floatfmt=".4f"))
- print("\nError Analysis:")
- print(f"MSE (Monte Carlo vs Quantum): {mse:.8f}")
- if __name__ == "__main__":
- np.random.seed(42)
- # First show numerical results
- analyze_bell_test()
- # Then show comprehensive visualization
- plot_comprehensive_analysis()
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