Numerical Validation of the NTU Coarse-Graining equation

A new numerical validation of the NTU coarse-graining equation has been completed.

This test represents an important milestone because it combines two previously independent developments:

  • the fractal thermodynamics framework developed by Queirós-Conde,
  • and the No-Time Universe (NTU) coarse-graining framework.

Both approaches independently converge toward the existence of an effective fractal dimension:Deff2.1D_{\mathrm{eff}} \simeq 2.1

Within fractal thermodynamics, this dimension characterizes the geometry of the quantum fractal paths.

Within the NTU framework, the same dimension naturally emerges from the fractal pilot surface generated by the pantographic transformation law acting on the pre-link substrate.

The numerical simulations were therefore performed using the common fractal coefficient:Deff2.1D_{\mathrm{eff}} \simeq 2.1

and the NTU surface law:Σ(N)=P2NDeff\Sigma(N) = \ell_P^2 N^{D_{\mathrm{eff}}}

where:N=λdBPN = \frac{\lambda_{dB}} {\ell_P}

The resulting quantum and gravitational evolution functions are:FQ=χP2NDeff+12F_Q = \chi\, \ell_P^2 N^{D_{\mathrm{eff}}+\frac{1}{2}}

andFG=(1χ)P2NDeff32F_G = (1-\chi)\, \ell_P^2 N^{D_{\mathrm{eff}}-\frac{3}{2}}

The simulations confirm that the discrete NTU evolution equation:Xn+1Xn=[χnFQ+(1χn)FG]ΔNTUX_{n+1} – X_n = \Big[ \chi_n F_Q + (1-\chi_n)F_G \Big] \Delta_{\mathrm{NTU}}

naturally converges toward the continuous stochastic description:dX=[χFQ+(1χ)FG]dt+χG0dWtdX = \Big[ \chi F_Q + (1-\chi)F_G \Big]dt + \chi G_0 dW_t

and subsequently toward the associated Fokker–Planck equation:Pt=X{[χFQ+(1χ)FG]P}+122X2[χ2G02P]\frac{\partial P}{\partial t} = – \frac{\partial} {\partial X} \left\{ \left[ \chi F_Q + (1-\chi)F_G \right] P \right\} + \frac{1}{2} \frac{\partial^2} {\partial X^2} \left[ \chi^2 G_0^2 P \right]

The numerical results reproduce the expected variance:Var(Xt)=χ2G02t\mathrm{Var}(X_t) = \chi^2 G_0^2 t

with excellent agreement between the discrete simulations and the continuous analytical prediction.

Perhaps more importantly, this validation provides a direct physical interpretation of the Brownian term.

In the NTU framework, stochasticity is no longer introduced as an external mathematical assumption. It emerges from the fraction of unresolved open pre-link configurations:χ=ΣopenΣopen+Σclosed\chi = \frac{\Sigma_{\mathrm{open}}} {\Sigma_{\mathrm{open}} + \Sigma_{\mathrm{closed}}}

The Brownian process therefore appears as the effective 4D projection of a deeper fractal geometry rather than as a fundamental property of nature.

This new result strengthens the convergence between fractal thermodynamics, stochastic descriptions of physical systems, and the NTU framework, while providing a complete mathematical pathway from discrete substrate dynamics to the continuous Fokker–Planck description observed in emergent spacetime.

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