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Study reconstructs light bending in hyperbrane relativity, indicating new insights on light behavior in gravity fields.
Overview This manuscript reconstructs the measured 1.75 arcsecond solar deflection of starlight within Hyperbrane Relativity (HBR), a geometric extension of general relativity in which the observable universe is modeled as a 3-brane translating through a flat, four-dimensional Euclidean bulk. Main Result In HBR, a mass is a localized push-out, or density enhancement, of the primary field ψbulk, and light is a transverse brane-section wave that refracts through this density. The weak-field refractive index n(r) = 1 - αΦN/c² is therefore treated as a single-channel optical response, not as a sum of separate temporal and spatial contributions. With α = 2 fixed by the Shapiro/Cassini bound γ = 1, the model reproduces δθ = 4GM/(c²b) ≈ 1.75 arcseconds. Epistemic Status Derived within HBR: the field ΦN and the single push-out refraction mechanism. Empirically fixed at present: the coefficient α = 2. Open Problem O55k: a first-principles local derivation of α = 2 from the ψbulk field equation. The familiar “second half” of the solar deflection is therefore not treated as a separate HBR effect. It is interpreted as the way general relativity’s two-component metric bookkeeping accounts for the same observable. Strong-Field Extension The same single-density ontology is extended to the Shapiro delay, the parametrized-post-Newtonian limit, and a strong-field verification programme for horizonless compact objects. In this extension, a BH-mimic is not tested by the presence of a ring image alone. Instead, it must satisfy an over-constrained signature predicted by one dispersive shielding shell: nonzero and chromatic central floor; chromatic ring-edge softening; polarization-dependent opacity; delayed low-frequency leakage; energy-budget closure. Throughout the manuscript, measured numbers are used only as final comparisons, never as inputs.
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yuichi yamamoto (2026) studied this question.
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