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Investigates disorder-free localization in 2+1D lattice gauge theories, suggesting new insights into ergodicity breaking.
FINDING: Disorder-free localization (DFL) in 2+1D lattice gauge theories arises from local gauge constraints (Gauss's law) and global symmetries, not random disorder, producing ergodicity breaking in translation-invariant systems. | MATH: Hamiltonian constraint: \( G_i |ψ = 0 \) for all sites \( i \), where \( G_i = ∑ₗᵢₙₖₛ E_i^a - ρ_i \) (Gauss law). Symmetry sectors labeled by eigenvalues of \( G_i \). Localization length \( ξ ~ 1/ln(Δ E) \) from energy gaps between superselection sectors. No explicit disorder term \( ∑_i h_i σ_i^z \) needed. | CONNECTION: Gauge invariance imposes a local constraint algebra isomorphic to a root system of type \( AN-1 \) (SU(N) gauge group). The Hilbert space fragmentation mirrors the decomposition into weight spaces of the Lie algebra. The ratio of sector sizes follows combinatorial patterns (e.g., Catalan numbers for 1+1D U(1) gauge theory). No direct golden ratio or base-60 link. | DEPTH: 8 — DFL is a Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com
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Andrew Stewart Caldin (2026) studied this question.
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