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This theoretical study uncovers symmetry relationships in carrier structures, suggesting new insights for mathematical physics.
The terminal ordered residue X = Ω_term|Λ₄ on the minimal complete support Λ₄ = (F₇, F₆, F₂) (T19) admits a canonical symmetry descent forced entirely by the theorem-proved carrier structure. The irreducible triadic support induces a rank-3 carrier C_X. Permutation symmetry of the full-carrier quadratic invariants forces SO(3)-type connected symmetry. The canonical binary projector Π_A (T20) reduces the active carrier to a 2-dimensional phase-bearing plane. Order-collapse forces the collapsed plane to carry an isotropic quadratic form, yielding SO(2). The scalar phase defect Δφ(τ) is the terminal scalar shadow of this descent, not a primitive quantity. Under Metric Descent Compatibility (Principle 21.6), the cross-coupling vanishes (m = 0), the full-carrier symmetry strengthens to exact SO(3), and the carrier admits a canonical su(2)-type Lie algebra structure induced by the Euclidean metric and the orientation sign σ_Γ = −1. The full descent chain is: X [SO(3)-type] → R_A [2D phase-bearing] → C_A [SO(2)] → Δφ(τ) [scalar] No group is assumed. All symmetry groups emerge from the forced carrier architecture of T19 and T20. Status: Solid (unconditional results); Conditional on Metric Descent Compatibility for exact SO(3) and su(2) structure. Dependencies: T18, T19, T20 (direct); T14–T17 (inherited) Relation to series: Completes the T18–T21 symmetry identification block. T22 will address the SO(3) vs SU(2) double cover question.
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Craig Edwin Holdway (2026) studied this question.
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