WOLFRAM NOTEBOOK

Sqrt[g(X)]
Cone is an integral of Sqrt[g] over the tube
Small t wrt radius of graph; large t wrt 1
Source of change in Sqrt[g] is divergence or convergence of geodesics
Ricci tensor: area of geodesic bundle
Weyl tensor: [trace free part of Riemann tensor]
1. Individual hyperedge
2. Space seems continuous
3.
4. Size of t he universe
Claim is that between scales 1 and 2, you have to have a perfect “geodesic monopole” to achieve correct dimensional space.
Nothing can cancel R t t. But the higher order terms could cancel in various ways.
Action verion:
R Sqrt[g]
Einstein-Hilbert action is:
bulk geodesic volume

Dimension extremization

Limits

Graph metric: distance along a hyperedge = 1
Physical metric: whole hypergraph is unit size (or 10^26 m), and the edges are scaled accordingly
[[ We could rescale our plots
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With each new t (or r) you want the growth rate to not differ from r^d
For large t, growth rate has to be t^(d+1)

Paths

If no refinement

[[Transitivity of geodesics ??]]

JG argument

t is in graph coordinates

Momentum

Pick a hypersurface
+ neighbors

Number of edges of causal graph slicing a hypersurface
[If the hypersurface is energy]


Momentum + energy are frame dependent.
Given a structure in causal graph:
purely timelike
Excess of edges in CG

[Derivative of excess of edges ???] <energy conservation?>

There are different ways to increase the number of hyperedges
Think about a buckyball....

Excess of edges due to energy is compensated by a decrease in edges due to positive curvature
Fixed energy density : 1 + δρ

Energy momentum

vacuum energy +
Projecting edges through spacelike surface

Continuum Limit

Foliations are the way we idealize the observer
[foliations are we turn reality into the subjective experience of the observer]
If we want a simple description of physics, need to have simple foliations

Quantum analog

Non-interacting branchial graph [ bunch of separated pieces without entanglement ] : free field case

Boost is like a transformation between observers


Basic indeterminancy: you can go either way on a critical pair. But entanglement in branchial graph.

Curvature measures entanglement because it is a sign of non-commutation

[x, p] = i

Go across the spatial graph and down the causal graph

Operators vs. states ....
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