Investigates the impact of a density-matrix formulation on cosmological models, suggesting novel implications for eternal universes.
This repository contains the fourth iteration of the Minimal Eternal Universe Theory (mEUT), an independent research project in theoretical cosmology. mEUT v4.0 proposes a singularity-free, eternal cosmological framework driven by the purely kinetic energy of a single real scalar field. Key Features of v4.0: Microscopic Derivation of Dissipation: Unlike previous versions, the dissipation parameter η is derived from first principles using the Nakajima-Zwanzig projection technique and the fluctuation-dissipation theorem, evaluated within a 64-vertex truncation of holonomy-corrected geometric operators. Density-Matrix Dynamics: The theory moves beyond simple wave-function evolution to a reduced density-matrix formulation (ρϕ), providing a more robust bridge between Loop Quantum Gravity (LQG) and effective Friedmann dynamics. Emergent Arrow of Time: The model provides a microscopic origin for the thermodynamic arrow of time through irreversible entropy production during the quantum bounce phase. Observational Signatures: Includes predictions for the suppression of the primordial power spectrum (PR(k)), offering a potential resolution to the S8 and H0 tensions. Contents: Numerical_Simulation_Data: Raw data from the 64-vertex truncation and large-j extrapolation. QuTiP_Scripts (optional if included): Python scripts used to solve the Lindblad master equation. import numpy as npimport matplotlib.pyplot as pltfrom qutip import * def run_mEUT_v4_complete(): print("Starte mEUT v4.0 Simulation...") # --- 1. System-Setup --- N = 60 # Hilbertraum-Dimension a = destroy(N) phi_op = (a + a.dag()) / np.sqrt(2) p_op = -1j * (a - a.dag()) / np.sqrt(2) # Hamiltonian: Rein kinetisch H = p^2 / 2 H = p_op**2 / 2 # --- 2. Dissipations-Profil eta(t) --- # Modelliert den Peak am Bounce (t=0) gemäß 64-Vertex-Modell def eta_func(t): return np.exp(-t**2 / 2.0) # --- 3. Zeitentwicklung (Lindblad) --- times = np.linspace(-5, 5, 400) psi0 = coherent(N, -3.0) # Pre-Bounce Zustand rho = ket2dm(psi0) entropy = [] states = [] # Wir simulieren schrittweise, um eta(t) dynamisch anzuwenden dt = times[1] - times[0] for t in times: states.append(rho) entropy.append(entropy_vn(rho)) # Lindblad-Update: d_rho = -i[H, rho]dt + eta(t) * L_dissipator(rho)dt eta = eta_func(t) L = p_op # Impuls als Jump-Operator (kinetische Dissipation) # Kommutator-Teil d_rho_ham = -1j * commutator(H, rho) # Dissipator-Teil (Lindblad-Form) d_rho_diss = eta * (L * rho * L.dag() - 0.5 * L.dag() * L * rho - 0.5 * rho * L.dag() * L) rho = rho + (d_rho_ham + d_rho_diss) * dt # --- 4. Visualisierung --- # FIG 1: Entropie und eta plt.figure(figsize=(10, 5)) plt.plot(times, entropy, 'r', label='v. Neumann Entropy S') plt.plot(times, [eta_func(t)*max(entropy) for t in times], 'b--', label='Dissipation eta (scaled)') plt.title('mEUT v4.0: Entropy & Dissipation') plt.xlabel('Relational Time phi') plt.legend() plt.savefig('entropy_plot.png') plt.show() # FIG 2: Wigner-Phasenraum-Evolution xvec = np.linspace(-7, 7, 150) indices = [0, len(times)//2, len(times)-1] # Start, Bounce, Ende titles = ['Pre-Bounce (Pure)', 'Bounce (Interacting)', 'Post-Bounce (Mixed/Classical)'] fig, axes = plt.subplots(1, 3, figsize=(15, 5)) for i, idx in enumerate(indices): W = wigner(states[idx], xvec, xvec) axes[i].contourf(xvec, xvec, W, 100, cmap='RdBu') axes[i].set_title(titles[i]) plt.savefig('wigner_plots.png') plt.show() print("Simulation abgeschlossen. Plots wurden gespeichert.") if __name__ == "__main__": run_mEUT_v4_complete()
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Karol Frank (2025) studied this question.
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