Holographic Quantum Simulation of Traversable Multi-Mouth Wormholes — E8 Intelligence Research

Andrew Stewart Caldin

Published Oct 4, 2026• 0 citations

Abstract

FINDING: Traversable wormhole construction in the lab via holographic quantum simulation (SYK model) and multi-mouth wormhole topology with free-group fundamental structure. MATH: - SYK model: ( H = \sum_{i Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com

DOI: 10.5281/zenodo.23131932

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Publisher

Abstract

DOI: 10.5281/zenodo.23131932

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\pi_1 = F_2

(free group on two generators) for the three-mouth case, with the topology described by a genus-2 handlebody; (4) the ER=EPR correspondence maps entangl Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com

\Delta t \propto 1/\mu

(inverse coupling strength). - Multi-mouth case (arXiv:2012.07821): fundamental group

\pi_1 = F_2

(free group on two generators) for three mouths — topology encoded in non-abelian group structure. - Key constant:

e^{S}

(entanglement entropy) sets wormhole throat size;

S \sim N

for SYK with

N

Majorana fermions. CONNECTION: - The free group

F_2

is the universal covering group of all crystallographic root sys Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com

J_{ijkl}

with random Gaussian distribution, variance

\langle J_{ijkl}^2 \rangle = 2J^2/(2N)^3

; the traversable wormhole requires a double-trace deformation

\delta H = \sum_{ij} g_{ij} O_i O_j

with

g_{ij} \propto \frac{1}{N} e^{i\mu(t_i-t_j)}

; the mutual information

I(A:B) = S_A + S_B - S_{AB}

must be positive and grows as

I \sim \frac{2\pi c}{3} \frac{\beta - t}{\beta}

for the teleportation signal; the multi-mouth case uses the free group

F_2

as the fundamental group, with the wormhole throat area quantized as

A \sim 4G\hbar \log(\text{rank})

; the time advance is

\Delta t \sim \frac{\beta}{2\pi} \log\left(\frac{1}{g}\right)

Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com