The CKM sector of the exceptional-Jordan programme: finite-Dirac mass moduli, two conditional angle estimates, and the weak-to-mass bridge
arXiv:2608.01445
Abstract
The Standard Model does not determine quark masses or the CKM matrix. In the exceptional-Jordan programme, square-root masses occupy short chains. Compressing the symmetric-cube lift onto occupied nodes gives a root-mass operator whose square yields the proposed mass ratios, packaging that spectrum and relative left frames in one finite Dirac operator without deriving the frames. Conditional on the transport, virtual-node-amplitude, real- and balanced-quadrature choices, the no-fit layer gives ( high) and ( high) at . The relation is a factor two low; one complex long edge is fitted. The two balanced orientations give branches and , so the former ratio is not robust and raw is convention-dependent. For an adopted -- family embedding, we construct an exact Peirce-changing Albert lift in , reproducing conjugate up/anti-down transport and . For an adopted cyclic Majorana placement and real-linear projection, its completion has real support while the quadrature vanishes; and or are compatibility results in this class. The minimal radial-quartic cyclic truncation has equal-magnitude full-rank extrema or a flat direction; a mixed Albert cubic gives stable alignment only in a chosen three-edge subspace. Six diagonal mass links plus three directed Peirce links would form a connected one-cycle nine-link graph if the Yukawa block is linear in the projected bridge. This is a candidate Arkani-Hamed et al. texture skeleton, not a derivation: family-vacuum selection, chiral projection and right-frame locking remain open.
33 pages, 2 tables; ancillary verification script included. Results v1-corrected relative to Zenodo record 10.5281/zenodo.21196380 (4 July 2026): sign error in the texture scan fixed, Layer-2 fit solved exactly on a coherent PDG 2024 target set; see footnote 1 for the change log