Randomized trial explores infall dynamics of Fano lattice with rotational interactions in black hole environments, suggesting new geometric insights.
The infall geodesic ODE governing the rotation of the Fano lattice tilt angle θ during radial free fall into a Schwarzschild black hole is derived and numeri- cally integrated. The ODE has a two-term structure: (1) a geometric term K(r) = −rs/(2r2p 1 −rs/r), the extrinsic curvature of the Schwarzschild constant-t hypersur- face in the Kruskal embedding, which rotates θ through ∆θgeo = 56.67; and (2) an interaction term α K(r) sin 2θ, coupling the geometric rotation rate to the current aux- etic shear state of the lattice, which contributes an additional ∆θint = 16.55. The full ODE is dθ/dr = K(r)[1 + α sin 2θ] with α = 0.40446, the Fano lattice material coupling to the Schwarzschild Weyl curvature. The ODE is integrated from θ(∞) = 4 (ambient Fano tilt) to θ(r− s ) = 77.218 (horizon limit), which equals arccos(p∗ e7) = arccos(0.22124) from the partition function of Paper XCV a non-trivial consistency check between the dynamical ODE and the statistical microstate count. At r = rs, a step function adds +12.78 discontinuously, taking θ from 77.22 to 90: this is the brane puncture (Paper XC), the sudden transition from brane-tangential to brane-orthogonal (bulk) motion. The total rotation is 86 = 90 −θG2, completing the full range from ambient Fano tilt to bulk-orthogonal. Three new predictions are made (P47P49). 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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