Expanding Wormhole Simulation with Majorana Particle

Backgrounds: Based on SYK-related models, Majorana particle is a fermion that is its own antiparticle. Recent discovery on simulating traversable wormhole by quantum processor based on Majorana particle is a significant progress in quantum simulation. By adding possible extendable approaches, more possibility could be suggested. Objectives: Discovering symmetry conservation attribute from Majorana particle to expand its usage for wormhole. Methods: By applying to the simplified non-unit model, additional considerations for simulating wormhole would be discovered. Results: Additional considerations of expanding holographic wormhole could be discussed in model.Backgrounds: Based on SYK-related models, Majorana particle is a fermion that is its own antiparticle. Recent discovery on simulating traversable wormhole by quantum processor based on Majorana particle is a significant progress in quantum simulation. By adding possible extendable approaches, more possibility could be suggested. Objectives: Discovering symmetry conservation attribute from Majorana particle to expand its usage for wormhole. Methods: By applying to the simplified non-unit model, additional considerations for simulating wormhole would be discovered. Results: Additional considerations of expanding holographic wormhole could be discussed in model.

Dec 24, 20220 citations

Jihyeon Yoon

Dec 7, 20220 citations

Expanding Wormhole Simulation with Majorana Particle

Jihyeon Yoon

Mar 17, 20230 citations

Expanding Wormhole Simulation with Majorana Particle

Jihyeon Yoon

Jun 7, 20230 citations

Holographic Wormholes in the Lab via SYK Quantum Simulation — E8 Intelligence Research

Andrew Stewart Caldin

FINDING: Traversable wormhole construction in the lab via holographic quantum simulation (SYK model) and multi-mouth wormhole topology with free group structure. | MATH: The key mathematical objects are: (1) the Sachdev-Ye-Kitaev (SYK) model — a 0+1D quantum mechanical model with N Majorana fermions and random all-to-all 4-body interactions, Hamiltonian $ H = \sum_{i 0 $ (negative energy injection); (3) for multi-mouth wormholes: fundamental group $\pi_1 = F_2$ (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.comFINDING: Traversable wormhole construction in the lab via holographic quantum simulation (SYK model) and multi-mouth wormhole topology with free group structure. | MATH: The key mathematical objects are: (1) the Sachdev-Ye-Kitaev (SYK) model — a 0+1D quantum mechanical model with N Majorana fermions and random all-to-all 4-body interactions, Hamiltonian $ H = \sum_{i 0 $ (negative energy injection); (3) for multi-mouth wormholes: fundamental group $ \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

Sep 7, 20260 citations

Holographic Wormholes: Quantum Simulations, Not Spacetime Tears — E8 Intelligence Research

Andrew Stewart Caldin

FINDING: Laboratory-created traversable wormholes are holographic quantum simulations (SYK model) of an eternal traversable wormhole geometry, not physical spacetime tears. | MATH: SYK model: $ H = \sum_{i \mu_c \sim T/\sqrt{N} $ (temperature $T$ , $N$ Majorana fermions). The holographic dual is JT gravity: $S = \frac{\phi_0}{16\pi G_N} \int \sqrt{g} R + \frac{1}{16\pi G_N} \int \phi(\sqrt{g}R + 2)$ . | CONNECTION: The traversability condition involves a phase transition at $\mu_c$ , and the mutual information between the two boundaries $I(A:B) = S_A + S_B - S_{AB}$ exhibits a sharp jump — a symmetry-b Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.comFINDING: Laboratory-created traversable wormholes are holographic quantum simulations (SYK model) of an eternal traversable wormhole geometry, not physical spacetime tears. | MATH: SYK model: $ H = \sum_{i \mu_c \sim T/\sqrt{N} $ (temperature $ T $, $ N $ Majorana fermions). The holographic dual is JT gravity: $ S = \frac{\phi_0}{16\pi G_N} \int \sqrt{g} R + \frac{1}{16\pi G_N} \int \phi(\sqrt{g}R + 2) $. | CONNECTION: The traversability condition involves a phase transition at $ \mu_c $, and the mutual information between the two boundaries $ I(A:B) = S_A + S_B - S_{AB} $ exhibits a sharp jump — a symmetry-b Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com

Oct 5, 20260 citations

\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

T

N

Majorana fermions). The holographic dual is JT gravity:

S = \frac{\phi_0}{16\pi G_N} \int \sqrt{g} R + \frac{1}{16\pi G_N} \int \phi(\sqrt{g}R + 2)

. | CONNECTION: The traversability condition involves a phase transition at

\mu_c

, and the mutual information between the two boundaries

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

exhibits a sharp jump — a symmetry-b Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com