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IndisputableMonolith.Gravity.CubicReggeProof

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Cubic-lattice bridge from discrete J-cost dynamics to continuum Einstein–Hilbert geometry. Gravity workers in the RS programme cite it for the linearized Euler–Lagrange identification with the lattice Laplacian and for controlled Regge-action convergence rates. The argument chains 3D continuum-limit lemmas with bond-wise action estimates and the identity that the derivative of cosh(ε)−1 is sinh(ε).

claimOn the cubic lattice $\mathbb{Z}^3$, the linearized Euler–Lagrange equation of the bond-wise $J$-cost action is equivalent to vanishing of the discrete Laplacian. Flat configurations satisfy the EL equations exactly. The total Regge action converges to the continuum Einstein–Hilbert action, with relative error tending to zero at a controlled rate as the lattice spacing shrinks.

background

Recognition Science gravity is built on the cost $J(x)=\frac12(x+x^{-1})-1$, uniquely minimized at $x=1$. In log coordinates this is $J(e^t)=\cosh(t)-1$, a convex bowl. DiscretenessForcing records that this landscape forces discrete structure; ContinuumLimit shows that long-wavelength discrete $J$-dynamics on $\mathbb{Z}^3$ yield a second-order diffusion equation of Klein–Gordon type.

LatticeConvergence extends the 1D second-order continuum limit to $D=3$ by writing the cubic Laplacian as a sum of three independent 1D Laplacians. ReggeCalculus supplies the exact nonlinear Regge framework on the RS lattice (edge lengths and deficit angles), replacing linearized deficit ansätze. NonlinearConvergence and ReggeConvergence record the inputs needed to pass from Regge action to Einstein–Hilbert geometry.

This module sits between those foundations and the packaged lattice–manifold correspondence. It introduces the bond-wise action, the Euler–Lagrange operator for that action, its linearization about flat space, and the continuum limit of the cubic Laplacian.

proof idea

The module is a chain of short analytic lemmas, not a single monolithic proof.

First, the elementary identity $d/d\varepsilon(\cosh\varepsilon-1)=\sinh\varepsilon$ (and $\sinh'(0)=1$) converts log-coordinate cost derivatives into hyperbolic functions. The Euler–Lagrange operator of the bond action is then written explicitly; flat configurations are checked to satisfy it.

Linearization about the flat point identifies the EL operator with the negative discrete Laplacian (equivalently, linearized EL vanishes iff the Laplacian vanishes). Separately, the action per bond is defined and summed; total-action convergence and a relative-error rate are proved so that the relative error tends to zero in the continuum limit. The cubic Laplacian continuum limit is imported from the lattice-convergence layer and tied to the linearized EL picture.

why it matters in Recognition Science

Without a cubic-lattice EL–Laplacian dictionary and controlled action convergence, the deformed-cubic-lattice story cannot be closed. Downstream, UnifiedLatticeManifoldCorrespondence packages the full claim: given a smooth Lorentzian $(M,g)$, there is a sequence of deformed cubic lattices whose Regge action converges to $S_{\mathrm{EH}}[g]$ and whose Regge equations converge to the Einstein field equations.

This module supplies the cubic, linearized, and rate ingredients that package needs. It sits on the gravity side of the forcing chain after $D=3$ (T8) and the eight-tick discrete structure, and it uses the $J$-cost uniqueness (T5) only through the hyperbolic log form already fixed upstream. It does not itself claim the full nonlinear curved-manifold correspondence; that is the parent module's job.

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