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import numpy as np
import pandas as pd
import json
import os
# Constants
c = 299792458 # Speed of light in m/s
E_mc2 = c**2 # Mass-energy equivalence in J/kg
TSR = E_mc2 / (1.38e-23) # Temperature to Speed Ratio in K/m/s
alpha = 1.0 # Proportional constant for TSR
Q = 2 ** (1 / 12) # Fractal structure parameter
dark_energy_density = 5.96e-27 # Density of dark energy in kg/m^3
dark_matter_density = 2.25e-27 # Density of dark matter in kg/m^3
collision_distance = 1e-10 # Distance for collision detection
Hubble_constant = 70.0 # km/s/Mpc (approximation)
Hubble_constant_SI = Hubble_constant * 1000 / 3.086e22 # Convert to SI units (s^-1)
# Initial conditions
temperature_initial = 1.0 # Planck temperature in K
particle_density_initial = 5.16e96 # Planck density in kg/m^3
particle_speed_initial = TSR * temperature_initial # Initial speed based on TSR
# Simulation time
t_planck = 5.39e-44 # Planck time in s
t_simulation = t_planck * 1e5 # Shorter timescale for simulation
# Particle masses (in GeV)
particle_masses = {
"up": 2.3e-3,
"down": 4.8e-3,
"charm": 1.28,
"strange": 0.095,
"top": 173.0,
"bottom": 4.18,
"electron": 5.11e-4,
"muon": 1.05e-1,
"tau": 1.78,
"photon": 0,
"electron_neutrino": 0, # Neutrinos have very small masses
"muon_neutrino": 0,
"tau_neutrino": 0,
"W_boson": 80.379,
"Z_boson": 91.1876,
"Higgs_boson": 125.1,
"gluon": 0, # Massless
"proton": 0.938,
"neutron": 0.939,
"pion_plus": 0.140,
"pion_zero": 0.135,
"kaon_plus": 0.494,
"kaon_zero": 0.498
}
# Conversion factor from GeV to J
GeV_to_J = 1.60217662e-10
# Simulation setup
num_steps = int(t_simulation / t_planck)
# Tunneling probabilities to investigate
tunneling_probabilities = np.arange(0.001, 1.5, 0.001) # Exclude 1.0
# Create a directory to store the data
data_dir = "big_bang_simulation_data"
os.makedirs(data_dir, exist_ok=True)
# Functions to incorporate relativistic effects and collisions
def relativistic_energy(particle_speed, particle_mass):
epsilon = 1e-15 # A small value to avoid division by zero
return particle_mass * c**2 / np.sqrt(max(1e-15, 1 - (particle_speed / c) ** 2 + epsilon))
def relativistic_momentum(particle_speed, particle_mass):
epsilon = 1e-15 # A small value to avoid division by zero
return particle_mass * particle_speed / np.sqrt(max(1e-15, 1 - (particle_speed / c) ** 2 + epsilon))
def update_speed(current_speed, current_temperature, particle_mass):
"""Update the speed of a particle based on temperature and mass."""
return TSR * current_temperature # Update speed using TSR
def check_collision(particle_speeds, collision_distance, current_step):
for j in range(len(particle_speeds)):
for k in range(j+1, len(particle_speeds)):
if np.abs(particle_speeds[j][current_step] - particle_speeds[k][current_step]) < collision_distance:
return True, j, k
return False, -1, -1
def handle_collision(particle_speeds, particle_masses, idx1, idx2, current_step):
"""Handle a collision between two particles."""
p1 = relativistic_momentum(particle_speeds[idx1][current_step], particle_masses[idx1])
p2 = relativistic_momentum(particle_speeds[idx2][current_step], particle_masses[idx2])
# Calculate velocities after collision using conservation of momentum
total_momentum = p1 + p2
total_mass = particle_masses[idx1] + particle_masses[idx2]
v1_new = (total_momentum / total_mass) * (particle_masses[idx1] / total_mass)
v2_new = (total_momentum / total_mass) * (particle_masses[idx2] / total_mass)
particle_speeds[idx1][current_step] = v1_new
particle_speeds[idx2][current_step] = v2_new
# Simulate the Big Bang with Dark Energy, Dark Matter, Tunneling, and Relativistic Effects
for tunneling_probability in tunneling_probabilities:
print(f"Simulating for tunneling probability: {tunneling_probability}")
# Initialize arrays for simulation
num_particles = len(particle_masses)
particle_speeds = [[particle_speed_initial] * num_steps for _ in range(num_particles)]
particle_temperatures = [[temperature_initial] * num_steps for _ in range(num_particles)]
particle_masses_evolution = [[mass * GeV_to_J] * num_steps for mass in particle_masses.values()]
tunneling_steps = [[False] * num_steps for _ in range(num_particles)]
particle_masses_array = np.array([mass * GeV_to_J for mass in particle_masses.values()])
for current_step in range(1, num_steps):
for j in range(num_particles):
# Update temperature based on expansion of the universe
particle_temperatures[j][current_step] = particle_temperatures[j][current_step-1] * (1 - Hubble_constant_SI * t_planck)
# Update speed using TSR
particle_speeds[j][current_step] = update_speed(particle_speeds[j][current_step-1], particle_temperatures[j][current_step], particle_masses_array[j])
# Apply tunneling effect
if np.random.rand() < tunneling_probability:
particle_speeds[j][current_step] = particle_speeds[j][0]
tunneling_steps[j][current_step] = True
# Check for collisions
collision_detected, idx1, idx2 = check_collision(particle_speeds, collision_distance, current_step)
if collision_detected:
handle_collision(particle_speeds, particle_masses_array, idx1, idx2, current_step)
# Calculate entropy using von Neumann entropy formula
for j in range(num_particles):
if particle_masses_array[j] == 0:
entropy = 0
else:
entropy = -particle_masses_array[j] * np.log1p(particle_masses_array[j])
# Update mass based on entropy
particle_masses_evolution[j][current_step] = particle_masses_evolution[j][current_step-1] + entropy / c**2
# Print calculated masses at the end of the simulation
print(f"Calculated masses at the end of the simulation using the von Neumann entropy (Tunneling Probability: {tunneling_probability}):")
for j, particle in enumerate(particle_masses.keys()):
print(f"{particle}: {particle_masses_evolution[j][-1] / GeV_to_J:.4e} GeV")
# Save data to JSON file
data_filename = os.path.join(data_dir, f"big_bang_simulation_data_{tunneling_probability:.2f}.json")
data = {
"tunneling_probability": tunneling_probability,
"particle_masses_evolution": particle_masses_evolution, # No need for tolist()
"particle_speeds": particle_speeds,
"particle_temperatures": particle_temperatures,
"tunneling_steps": tunneling_steps
}
with open(data_filename, "w") as f:
json.dump(data, f)
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