codex
30 lines
2.8 KiB
Markdown
30 lines
2.8 KiB
Markdown
# The Emergence of the Minkowski Metric from Causal Sets via Thermodynamic Action Penalties
|
|
|
|
**Target Venue:** *Entropy*
|
|
|
|
## Abstract
|
|
Deriving the Minkowski metric from discrete graphs requires overcoming the Kleitman-Rothschild (KR) order collapse. A generic causal set overwhelmingly favors non-manifold KR-orders (e.g., three-layer structures). We formulate the Intellecton Lattice as a directed causal set and introduce a thermodynamic partition function governed by the Benincasa-Dowker action augmented with a local volume penalty. This partition function explicitly suppresses KR-orders, inducing a thermodynamic phase transition that heavily favors manifold-like geometries in the continuum limit. Consequently, the pseudo-Riemannian metric $SO(1, D-1)$ and the Poincaré algebra are shown to rigorously emerge as the macroscopic thermodynamic ground state of discrete causal interactions.
|
|
|
|
## 1. Introduction
|
|
A simple unweighted graph Laplacian yields a positive-definite Riemannian metric. To recover Lorentz invariance, we use a Causal Set. However, Causal Sets generically collapse into non-manifold structures.
|
|
|
|
## 2. The Partition Function and KR-Order Suppression
|
|
Let the network be a causal set $C$ representing the partial ordering of agent updates.
|
|
To extract the continuous metric signature, we evaluate the system statistically using the partition function:
|
|
$$
|
|
Z = \sum_{C} e^{-S_{BD}(C) - \beta V(C)}
|
|
$$
|
|
where $S_{BD}(C)$ is the discrete Benincasa-Dowker action, and $V(C)$ is a non-local volume penalty that counts the number of localized intervals. The parameter $\beta$ acts as an inverse topological temperature.
|
|
|
|
## 3. The Emergence of the Minkowski Metric
|
|
At low topological temperatures (high $\beta$), the volume penalty $\beta V(C)$ thermodynamically suppresses the highly entropic, non-manifold Kleitman-Rothschild orders.
|
|
The system undergoes a phase transition into a manifold-like phase where the continuum limit of the Benincasa-Dowker action yields the Einstein-Hilbert action over a pseudo-Riemannian manifold.
|
|
Because the surviving geometries rigorously preserve the causal precedence of the directed graph, the continuum limit metric tensor $g_{\mu\nu}$ natively possesses the minus sign required for Lorentz invariance. The Poincaré symmetry group $SO(1, D-1)$ is therefore derived as the thermodynamic limit of the augmented causal set.
|
|
|
|
## 4. Conclusion
|
|
Relativistic spacetime and the Minkowski metric emerge neither from classical graphs nor generic causal sets, but specifically from the thermodynamic ground state of causal graphs governed by volume-penalized discrete actions.
|
|
|
|
## References
|
|
1. Benincasa, D. M. T., & Dowker, F. (2010). *The Scalar Curvature of a Causal Set*. Physical Review Letters.
|
|
2. Surya, S. (2019). *The causal set approach to quantum gravity*. Living Reviews in Relativity.
|