Considering Counting Triangles to Unveiling Temporal Waves

  Considering Counting Triangles to Unveiling Temporal Waves By: John Gavel For years, my work in Temporal Flow Physics (TFP) has pursued a radical idea: what if spacetime itself —with all its gravitational curves and quantum fluctuations—isn't fundamental at all? What if it emerges from a deeper reality: a network of one-dimensional temporal flows , weaving the universe together moment by moment? It’s bold, yes—but I believe this view holds the key to a truly unified theory of physics , one that roots both quantum mechanics and gravity in the same temporal fabric. From Counting Triangles to Counting Time My earliest simulations: I counted triangles. More specifically, I measured how triangular motifs in temporal flow networks dissipated under coarse-graining. The decay rate of these patterns—captured by a parameter I called A₃ —served as a stand-in for emergent gravitational effects. If motifs faded predictably with scale, it suggested that macroscopic structure (like sp...

Linear progression scalar to vector

 Coupled interactions and vector-like dynamics within the Independent Asymmetrical Determinate Systems (IADS) subsets of this cellular automaton system:

Symmetrical Determinate System (SDS):

A one-dimensional array of points P = {p1, p2, ..., pn}

Each point pi has a scalar value vi

Uniform rules apply across the SDS


Independent Asymmetrical Determinate Systems (IADS):

Subsets Pk ⊂ P, each governed by a rate ri

These subsets exhibit coupled interactions as ri increases


Limits and Rates:


Limit L: A constant parameter that restricts the maximum range of value transfer

Rate ri: A variable parameter that determines the influence of neighboring points within an IADS subset


Coupled Dynamics:


For a point pi within an IADS governed by rate ri:


When ri = 1:

vi(t+1) = vi(t) + f(vi(t))

The value at pi depends only on its current value

When ri > 1:

vi(t+1) = vi(t) + Σ(j=-L to L) wij * f(vi+j(t))

wij represents the weight/influence of neighboring point pi+j on pi

f(vi+j(t)) describes the contribution of vi+j to the new value of vi


Weight Function:


wij = 1/ri for |j| ≤ L

As ri increases, neighboring points have more influence on vi

Example with Vector-Like Dynamics:

For pi with vi = 4, ri = 3, L = 2:

vi(t+1) = vi(t) + 1/3 * (f(vi-2(t)) + f(vi-1(t)) + f(vi(t)) + f(vi+1(t)) + f(vi+2(t)))

The future value of vi is influenced by its own current value and its 2 immediate neighbors


General Formula:


For pi in an IADS:

vi(t+1) = vi(t) + 1/ri * Σ(j=-L to L) f(vi+j(t))

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