Admissibility frontier · Edition 3

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Spin(2,3) Global Path Selection v20: Both Spin-Two Escapes Are Non-Identifiable

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corpus/programmes/closure/spin23-gravity-route/global-path-selection-v20.md
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  1. Spin(2,3), the Standard Model, and Furey: document map
  2. Both Healthy Spin-Two Escapes Are Inverse-Degenerate and Decoupled from Axial Selection
  3. Spin(2,3) Global Path Selection v20: Both Spin-Two Escapes Are Non-Identifiable

Spin(2,3) Global Path Selection v20: Both Spin-Two Escapes Are Non-Identifiable

Frozen: 23 October 2026

Both explicit healthy escapes from the finite local spin-two pole problem have now been matched back to local curvature data. Neither inverse problem is unique, and neither contains the axial vertex.

IDPathStateResult or blocker
ENZero-free entire completioncompletedinfinitely many functions share the pole count and \(p^4\) coefficient
BMPositive-residue bimetric completioncompletedfixed local coefficient determines only \(\tan^2\theta/m_2^2\)
CSCurvature data select the UV parentrejected as selectorboth inverse maps have continuous degeneracies
ASSpin-two parent selects \(1/8\)rejected as selectoraxial vertex is absent from both matching equations
NQComplete enlarged quantum parentexternally blockedparent principle, nonlinear consistency, positivity, flow and matching absent
SVStabilized torsional compactificationexternally blockedmicroscopic vacuum data absent

The spin-two problem admits healthy enlarged solutions, but the low-energy packet cannot choose among them or determine the torsion-fermion coefficient. Further progress requires a parent principle with genuinely cross-sector Ward relations, or the independent stabilized compactification construction.

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node verification/verify/verify_spin23_entire_completion_matching_degeneracy.mjs
node verification/verify/verify_spin23_bimetric_matching_degeneracy.mjs
node verification/verify/verify_spin23_new_model_path_selection_v8.mjs

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