Asymptotic su(2)-Isotropy of the Effective Quadratic Form and the Identification A_H = 2

Q10 proves that character-independence of the large-$q$ limit forces su(2)-isotropy of the effective quadratic form on $H_\mathrm{eff}$, and identifies the unique su(2)-isotropic quadratic form as the Casimir with value $A_H = 2$.

Overview

The Q7 bridge condition requires two asymptotic isotropy identifications: $A_Z = 2$ (established by Q8) and $A_H = 2$ (the subject of Q10). The second identification concerns the effective quadratic form on the horizontal subspace $H_\mathrm{eff}$ of the Heisenberg–Weil representation.

Q10 proves that, under spectral universality [U] (itself proved by U1), the character-independence of the large-$q$ limit forces su(2)-isotropy of the effective quadratic form. The unique su(2)-isotropic quadratic form on a two-dimensional irreducible representation is the Casimir, which takes the value 2.

Together with Q8 ($A_Z = 2$) and U1 (proof of [U]), Q10 closes the asymptotic isotropy condition $A_H = A_Z = 2$ entering the Q7 bridge, enabling the passage from spectral data to the emergent co-metric coefficients.

Status. Structurally motivated, conditional on [U] (proved by U1).

Core contributions

Role in the asymptotic isotropy chain

The Q7 bridge establishes a formal connection between admissibility data and emergent geometric coefficients, but requires as input the equality $A_H = A_Z$. The papers Q8 and Q10 supply this input from two independent directions:

The agreement $A_H = A_Z = 2$ is not postulated but derived from independent structural arguments, providing a consistency check internal to the spectral admissibility programme.

Dependence on [U]. The argument of Q10 is conditional on hypothesis [U], which is proved by U1 with rate $\varepsilon(q) = O(q^{-1/2})$.

Relation to the Cosmochrony programme

Q10 is a key node in the derivation chain leading from spectral admissibility to the identification of the effective Lorentzian co-metric. Its result feeds directly into Q11, which closes the temporal coefficient $A_\tau = 2$ and thereby identifies the full Minkowski co-metric $g^{\mu\nu} \propto \eta^{\mu\nu}$.

The full chain through which the metric emerges reads: Q5a → Q5b → Q7 → Q8 → Q9 → Q10 → U1 → W1 → H2 → Q11.

References

Jérôme Beau. Asymptotic su(2)-Isotropy of the Effective Quadratic Form and the Identification A_H = 2, 2026. doi:10.5281/zenodo.19880900