Skip to content
DraconiticResearch
Search Sources API
194,220 studies31 sourcesUpdated 26 min ago
PreprintCC BY-NC-ND 4.0arXiv

Descartes Curvature Geometry, Compact-Cycle Amplitudes, and the GST Cabibbo Seed

Abstract

Several apparently distinct formulations of the charged-lepton mass relation p2/e12 = 2/3 share a common algebraic object: the ratio of flavor-breaking to flavor-symmetric amplitude components on an internal family space. We show that (i) the relation expressed as a Fourier-mode constraint on Shulga's compact cycle, (ii) the same relation as a Descartes curvature condition in the sense of Kocik, and (iii) the Soddy completion of the resulting circle configuration are related by exact algebra, with no approximations. The Soddy completion defines a companion scale F2 = α2 μ⋆ with α= √(3/2) − 1 and μ⋆ = ∑ℓ mℓ; identifying this scale with m̅MSs(μ⋆) yields a light-quark mass cascade with the ratio md/ms = 5/2 − √6. Combined with the leading Gatto-Sartori-Tonin relation, this gives the down-sector Cabibbo seed √(md/ms) = √(3/2) − 1 = 0.22474…, numerically close to the measured |Vus| = 0.22503 ± 0.00068 (0.4σ). A full CKM evaluation requires the up-sector phase correction, which we defer. The correspondence is testable by future lattice QCD+QED determinations of md/ms; explicit failure modes are listed.

Versions

Related

  1. Five-dimensional Geometry from Spinning Amplitudes
    Lucile Cangemi, Iustin Surubaru
    arXivPreprintarXiv licenceFull textGravitation & general relativityHigh-energy & particle physicsarXiv
  2. Five-dimensional geometry from spinning amplitudes
    Lucile Cangemi, Iustin Surubaru
    Journal of High Energy PhysicsPeer-reviewedCC BY 4.0Full textHigh-energy & particle physicsCrossref
  3. Scattering amplitudes from geometry of kernel-free functionals on piecewise random null paths with memory
    Hiren Kakkad, Piotr Kotko
    arXivPreprintarXiv licenceFull textHigh-energy & particle physicsarXiv
  4. Transverse geometry reshapes current and tracer fluctuation amplitudes in quasi-one-dimensional single files
    Olivier Bénichou, Aurélien Grabsch
    Reports on Progress in PhysicsPeer-reviewedCC BY 4.0Full textCondensed matterStatistical & nonlinear physicsHALarXiv
  5. Weighted Berry curvature and global geometry of mixed quantum states
    Dominik Kuczyński, Erik Sjöqvist
    arXivPreprintarXiv licenceFull textCondensed matterQuantum physics & quantum informationarXiv
BibTeX
@misc{brilliant2026descartes,
  title = {{Descartes Curvature Geometry, Compact-Cycle Amplitudes, and the GST Cabibbo Seed}},
  author = {Andrew M. Brilliant},
  howpublished = {arXiv},
  year = {2026},
  month = oct,
  doi = {10.48550/arxiv.2610.36960},
  eprint = {2610.36960},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2610.36960},
  note = {CC BY-NC-ND 4.0},
}
RIS
TY  - UNPB
TI  - Descartes Curvature Geometry, Compact-Cycle Amplitudes, and the GST Cabibbo Seed
AU  - Andrew M. Brilliant
PY  - 2026
DA  - 2026/10/27
PB  - arXiv
DO  - 10.48550/arxiv.2610.36960
UR  - https://arxiv.org/abs/2610.36960
AB  - Several apparently distinct formulations of the charged-lepton mass relation p_2/e_1^2 = 2/3 share a common algebraic object: the ratio of flavor-breaking to flavor-symmetric amplitude components on an internal family space. We show that (i) the relation expressed as a Fourier-mode constraint on Shulga's compact cycle, (ii) the same relation as a Descartes curvature condition in the sense of Kocik, and (iii) the Soddy completion of the resulting circle configuration are related by exact algebra, with no approximations. The Soddy completion defines a companion scale F^2 = α^2 μ_⋆ with α= √(3/2) − 1 and μ_⋆ = ∑_ℓ m_ℓ; identifying this scale with m̅^MS_s(μ_⋆) yields a light-quark mass cascade with the ratio m_d/m_s = 5/2 − √6. Combined with the leading Gatto-Sartori-Tonin relation, this gives the down-sector Cabibbo seed √(m_d/m_s) = √(3/2) − 1 = 0.22474…, numerically close to the measured |V_us| = 0.22503 ± 0.00068 (0.4σ). A full CKM evaluation requires the up-sector phase correction, which we defer. The correspondence is testable by future lattice QCD+QED determinations of m_d/m_s; explicit failure modes are listed.
ER  -