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Spin(2,3) Global Path Selection v5: Coherent Nuclear Response

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corpus/programmes/closure/spin23-gravity-route/global-path-selection-v5.md
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  1. Spin(2,3), the Standard Model, and Furey: document map
  2. Coherent Nuclear Response Exhausts the Public Experimental-Hadronic Route
  3. Spin(2,3) Global Path Selection v5: Coherent Nuclear Response

Spin(2,3) Global Path Selection v5: Coherent Nuclear Response

Frozen: 23 October 2026

Reopening and correction

Version 4 treated a numerical electron-proton curve as a possible second nucleon input. The 30-microeV proton point is analytically recoverable from the published \(^{21}\mathrm{Ne}\) spin fractions, but the deeper result is that the proton and neutron curves share one likelihood. They are alternative one-coupling projections of one coherent nuclear response.

IDPathStateResult or blocker
EPXu proton pointcompleted\(|y_ey_p|\lesssim3.4752\times10^{-8}\) at 30 microeV
JXSimultaneous Xu responsecompleted\(c_n+0.0689655c_p\); blind line \(c_p=-14.5c_n\)
2IAdd \(^{129}\mathrm{Xe}\) directioncompletedrank two, but 2.204-degree separation and \(\kappa=52.38\)
2CPrecision two-isotope inversionexternally blockedjoint numerical likelihoods and nuclear covariance
H3Third quark projectionexternally blockedobservable outside the proton-neutron span
UVParent flavor predictionexternally blockedmatched UV Wilson coefficients

Decision

For simultaneous torsion coefficients the Xu experiment constrains

\[ {A\over|c_e|\,|c_n+0.0689655c_p|} >8.00195\times10^5\ {\rm GeV}^2. \]

Under the positive universal benchmark, proton and neutron contributions add and revise the conditional result to \(\sqrt A>72.401\) GeV. For general coefficients they can cancel exactly.

The existing \(^{129}\mathrm{Xe}\) experiment supplies a different isotope direction in principle. With a selected detailed shell-model spin fraction, the neon-xenon response matrix is full rank, but its condition number 52.38 makes inversion highly sensitive to experimental and nuclear-model errors.

Stopping status

The selected public experimental-hadronic route is exhausted at reproducible numerical depth. A defensible next calculation cannot be obtained by dividing published upper-limit curves. It requires common-mass joint likelihoods or response tables and nuclear-spin covariance. Even successful nucleon tomography leaves the exact third light-quark direction for a new observable or UV flavor relation.

Reproduction

node verification/verify/verify_spin23_xu_electron_proton_bound_map.mjs
node verification/verify/verify_spin23_xu_simultaneous_nucleon_coupling_map.mjs
node verification/verify/verify_spin23_two_isotope_nucleon_tomography.mjs
node verification/verify/verify_spin23_experimental_hadronic_path_selection_v5.mjs

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