Mathematical analysis demonstrates a conditional three-dimensional neutral sector from an SU(2) spinor carrier, indicating the admissibility threshold remains an open selection rule.
O21 defined the observable shell n₃ by the threshold Σc(n₃) = 3 and used it as structural input. This paper determines the exact status of the value three. The positive result is conditional: if the admissible neutral sector is carried by an irreducible two-dimensional SU(2)-valued Vρ C², its traceless neutral sector is su(2) Im\,H, of real dimension exactly three. Two bridges separate this theorem from a derivation of the threshold, and both are open. On the first, carrier selection, the paper determines what one candidate source supplies. The fingerprint vectors of the deposited O12 filtration are pure Fourier modes, so every proper level is a coordinate subspace with single-line Weyl support, and the exact stabiliser of that level in the Weil image of SL(2,Z/qZ) is U Mₙ, inside a Borel subgroup. This excludes the exceptional binary polyhedral groups $2T$, $2O$ and $2I$ at every proper level, including at primes where they exist in the ambient group. It does not exclude a spinor carrier: at explicit generic levels at $q = 53$ and $q = 101$ the stabiliser is Dicq, whose restricted Weil module is multiplicity-free, one character plus four inequivalent two-dimensional irreducibles, exactly two of them faithful and SU(2)-valued. The source therefore supplies genuine spinorial content, and the difficulty is selection, not existence. It splits in two: selecting which prime, block and depth the projection singles out within the generic filtration, which nothing here addresses; and, inside a level already known to be dicyclic, choosing between the two admissible carriers, for which a structurally motivated candidate — the unique odd member of Σ, q - cΣ\ — succeeds on all $17$ audited instances over $13$ distinct subspaces, with one step observed and not proved. The second bridge is observable identification: no theorem identifies the cumulative Gram–Schmidt span Σc with the dimension of the neutral traceless module, so the threshold remains a supplied selection rule. A caution accompanies the positive result: in the faithful two-dimensional representation of Q₈ the set \, \ generates the group with only two generator axes. The ADE observation of three eigenvalue classes is retained as a consistency check, not as evidence.
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Jérôme Beau (2026) studied this question.
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