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June 17, 20260 citationsOpen Access

Paper CCXXXIII: One-Octonion Ringdown Mode Content as the Akivis–Mal'tsev BCH Commutator Tower of Coalescing G2 Infundibula:

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BJBharathi Jagadeesan

Key Points

  • The primary aim is to investigate the cubic quasinormal mode amplitude predictions and their validation through direct measurements, correcting prior assertions.
  • Direct measurement on the Dyer & Moore CCE catalog (identified with SXS:BBH_ExtCCE:0010/0011/0012).
  • Validation of predictions against known quadratic modes and establishing a hierarchical structure in ringdown analysis.
  • Utilization of Bayesian data-driven identification methods for quasinormal mode content.
  • The cubic amplitude prediction was corrected from 1.255×10⁻² to approximately 0.595, fitting within the expected range.
  • Confirmed overtones extend to n=6, with cubic modes and retrograde configurations observed in specific spin states.
  • Five zero-parameter predictions were established regarding amplitude ratios, truncation indexes, and scaling laws for retrograde modes.

Abstract

v2 (2026-06-14) — ERRATUM appended. The headline cubic-QNM amplitude prediction η₃ = |C (2, 2, 0) ³|/|C (2, 2, 0) |³ = n·fbulk = 1. 255×10⁻² is FALSIFIED by direct measurement on the public Dyer single power of fIII = coherence, the same Born-once principle that fixes fIII in the neutrino sector; bulk fraction via the H⁻ associator e4, e5, e6=−2e7 → e7). The cubic is the unique framework nonlinear mode; quadratics are incomplete (2-of-3-dimension) projections = ordinary GR mode-coupling, carrying no framework prediction. The cubic mode’s existence and (6, 6) localization, the Fano quadratic selection rule, the retrograde-spin rule, and nₘax stand. See appended erratum + correction note. v2 (2026-06-14) — ERRATUM appended. The headline cubic-QNM amplitude prediction η₃ = |C (2, 2, 0) ³|/|C (2, 2, 0) |³ = n·fbulk = 1. 255×10⁻² is FALSIFIED by direct measurement on the public Dyer an attempted “all quadratics = n·fIII” generalization was tested and failed. The cubic mode’s existence and (6, 6) localization, the Fano quadratic selection rule, the retrograde-spin rule, and nₘax stand. See appended erratum + correction note. Pipeline validated against the known quadratic (2, 2, 0) ²→ (4, 4) ratio. Dyer nested Lie-bracket structure ↔ quadratic and higher multi-mode sourcings; octonion associator e4, e5, e6=−2e7 (Paper CVIII) ↔ the cubic mode (2, 2, 0, +) 3. Five zero-parameter predictions follow: (CCXXXIII-1) the cubic-to-fundamental amplitude ratio is the non-associative three-body coupling K/J = n·fbulk = 1. 255% already derived in Paper CXCVIII; (CCXXXIII-2) quadratic mode amplitude ratios follow the Fano-line incidence structure constants 2εijk; (CCXXXIII-3) the overtone tower truncates at nmax=5 from the G2 Cartan depth, with an n=6 recurrence corresponding to the free e7 radial breathing mode of Paper CCXIII; (CCXXXIII-4) retrograde-mode amplitude in anti-aligned-spin binaries scales as sin2 (θmisalign/2) from H+/H− ordering reversal (Paper CXLIX) ; (CCXXXIII-5) the framework predicts a late-time power-law tail of amplitude ∝ a0·M·t in Cauchy-characteristic matching simulations, pre-registered before any such catalog publishes such a measurement. The paper closes a triangle between Paper CCIX (BCH Taylor expansion of spacetime), Paper CCXIII (Onsager 6, 3 disk lock-in), and the GW birefringence prediction of Paper CCXXXII into a unified Lie-algebraic description of ringdown. Part of the One-Octonion Brane-Bulk Framework series. Anchor DOI: 10. 5281/zenodo. 19120873. Community: one-octonion-brane-bulk. Author: Bharathi Dasan Jagadeesan, M. D. , University of Minnesota. ORCID: 0000-0002-1143-941X.

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Cite This Study

Bharathi Jagadeesan (2026) studied this question.

synapsesocial.com/papers/6a323d57d50b63ecad207119https://doi.org/10.5281/zenodo.20695344
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Also Consider

Synapse has enriched 5 closely related papers on similar clinical questions. Consider them for comparative context:

  1. 1Paper CCXXXIV: One-Octonion Mode-by-Mode Projection of the Akivis–Mal'tsev BCH Tower onto the Kerr Spin-(−2) Spheroidal Basis:2026
  2. 2Paper CCXXXIII of the One-Octonion Brane-Bulk Series Ringdown Mode Content as the Akivis–Mal'tsev BCH Commutator Tower of Coalescing G2 Infundibula:2026
  3. 3Paper CCXXXIV of the One-Octonion Brane-Bulk Series Mode-by-Mode Projection of the Akivis–Mal'tsev BCH Tower onto the Kerr Spin-(−2) Spheroidal Basis:2026
  4. 4Paper CCXXXV: One-Octonion Preliminary Empirical Confirmation of the Akivis–Mal'tsev BCH Ringdown Predictions (Papers CCXXXIII + CCXXXIV) against the Dyer & Moore (PRL 136, 191403, 2026) Public2026
  5. 5Paper CCXXXV of the One-Octonion Brane-Bulk Series Preliminary Empirical Confirmation of the Akivis–Mal'tsev BCH Ringdown Predictions (Papers CCXXXIII + CCXXXIV) against the Dyer & Moore (PRL 136, 191403, 2026) Public2026