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FINDING: Phase transitions exist that cannot be described by Landau's spontaneous symmetry breaking paradigm — deconfined quantum critical points (DQCP) and topological transitions proceed without any local order parameter or hidden symmetry breaking. | MATH: Landau free energy F = F₀ + a(T−T_c)φ² + bφ⁴ + ...; order parameter φ transforms under symmetry group G → subgroup H. DQCP: no such φ exists; criticality governed by emergent gauge fields and fractionalized excitations. Order parameter scaling: ⟨φ⟩ ~ (T_c − T)^β with β from universality class. Topological transitions: no local order parameter; characterized by topological invariants (Chern number C ∈ ℤ, Z₂ index ν ∈ {0,1}). | CONNECTION: Topological invariants are integer-valued (Chern numbers, winding numbers) — discrete, not continuous ratios. No direct 0.618/1.618 connection in these findings. However: crystallographic symmetry breaking (Landau) maps to root systems and lattice structures; topological phases connect to Brilloui 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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