Explores the 12C(p, d) reaction mechanisms in eta' mesic nuclei, indicating new insights into particle interactions.
The 12C(p, d) reaction near the η′ emission threshold has recently been measured in coincidence with high-momentum backward protons by Sekiya et al. (PRL, DOI 10.1103/6vsl-ng7x, 2026, "Featured in Physics"), yielding the first direct detection of η′-mesic nuclei with bound-state structures at Eex −E0 = −30 MeV (1s) and −6 MeV (2p), V0 = −61 ± 1(stat) ± 5(syst) MeV, and local significance 3.5σ. Paper CXC of the One-Octonion Brane-Bulk Framework predicted the existence of these bound states from a winding-number formula mη′ = Nw¯hc/Lmax(KQ) with Lmax = 3 × spine = 1.7634 on the genus-3 warped Klein Quartic, exactly reproducing mη′ = 957.8 MeV at ΛQCD = 200 MeV. Paper CXC explicitly flagged the geometric identification of the segment 0.5878 as an open question. We resolve this question: in the warped Klein quartic metric (where the brane fabric carries the G2 long-root structure rather than the canonical hyperbolic metric of constant curvature K = −1), spine = arccosh(3)/3 = 0.5876, exact to 0.04%, where the factor of 3 is the square of the G2 long-root length, ( √ 3)2 = 3 — this is the warping factor itself. Each spine hop is one G2 long-root edge (ei →e7) on the 7,3-tiled warped Klein quartic; the η′ geodesic is exactly three such edges traversing the three handles of the Klein Quartic (Trinion 1 →2 →3 →4, i.e., u/d quark sector →c/s →t/b →leptons). The 12C(p, d) →η′-11C reaction is therefore identified as a three-long-root geodesic across the warped Klein quartic, with the warping factor 3 supplied by the G2 long-root length. Standard mathematical literature values for the unwarped Klein quartic (e.g., Schmutz Schaller's standard-metric systole) do not directly apply: the G2-warped metric is distinct from the canonical hyperbolic metric, and warped geometric quantities (warped systole 2 arccosh(7/2) = 3.8497, warped spine arccosh(3)/3 = 0.5876) are the framework-relevant ones. We discuss reconciliation with Sekiya et al.: the framework's ∆mη′ = −117 MeV at ρeff = 0.5ρ0 (Paper CXC) is ∼4× deeper than Sekiya's best-fit option B (V0 = −62 MeV) but consistent with Sekiya's option A (V0 = −110 MeV, W0 = −20 MeV), which the current data disfavor on χ2 grounds but cannot exclude given 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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