Two Axes, One Sky

The author supplied the definition on October 27, 2026: the axis is the ring of twisted light at the seam's middle. A study of the ring formalized it and priced the ring: J_ring = ħ · q_post/2 ≈ 2.64 × 10³⁶ ħ (q_post ≈ 5.28 × 10³⁶, the post-crossing count), as reported by the ring study from named film mechanics with no fitted parameter; that study's derivation is cited in §2, not reproduced here, and §2 prints the factor-of-two family uncertainty that governs the precision this number earns. Three forms of the amplitude map ξ(J) stood examined: the share, the response, and the flux. One more form, called C' here, died in that study by its own numbers. What waited was the choice. The author declares it: ξ(J) is the share, ξ_A(J) = J/J_ring on ring modes. This paper states that declaration and prints the full field around it. The response stands as the priced runner-up, with its imprint reading intact: at the sky it answers s_MW = 9.498 × 10⁴⁵, so galaxies cannot source the axis, and a world where the response is the map is a world where the axis was frozen in at the crossing. The flux stands named and uncomputable: its objects belong to a theory of the tube that has not been built. C' stands dead, for the reason given in §3. The sky chapter is honest in full. The specimens sit about 35-37 orders below the ring on the quantum side and about 39-66 orders above it on the sky side, and no named mechanism crosses the middle. The EB amplitude has not been produced: the share at ħ sits -34.207 dex under the target, the seam response +1.416 dex over it. The arithmetic among this paper's headline numbers was checked by script where checkable, and every checked identity reproduces; the film-mechanics derivation behind q_post was not re-run and stands as the ring study's reported result.