Manuscript IV@1 · IV.tex · figure · 351cb2d7

Exterior curvature witness

Model 3: scalar stress form and exterior record › A compact exterior curvature current · lines 3095–3135

IV@1#fig:exterior-curvature-witness

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gravitationalscalaroperator / instrumenterror / restrictionsupport / scope
(a)Uncut spacetime support
t|x|x*ψ
schematic. Scalar support ∣x∣≤r0+∣t∣|x|\le r_0+|t|. ψ\psi sits outside that cone.
(b)Curvature certificate
jij(0,x)=E4π∣x∣δijj_{ij}(0,x)=\frac{E}{4\pi|x|}\delta_{ij}
R1212(1)(j)(0,x∗)=E4πr∗3>0R^{(1)}_{1212}(j)(0,x_*)=\frac{E}{4\pi r_*^3}>0
d=∫ψR1212(1)(j)>0d=\int\psi R^{(1)}_{1212}(j)>0
(c)Conserved current
nonzero entries of JψJ_\psi only
∂μJψμν=0\partial_\mu J_\psi^{\mu\nu}=0
∫Jψh=∫ψR1212(1)(h)\int J_\psi h=\int\psi R^{(1)}_{1212}(h)
Momentum cutoff destroys exact compact spatial support. Only the pairing transfers: dΛ≥d/2d_\Lambda\ge d/2 for a selected finite Λ\Lambda, not the exterior pointwise separation.

Exterior curvature witness for Model 3. A radial compact scalar preparation produces positive initial exterior curvature, giving a positive compact conserved-current pairing on a short future slab. Coherent expectation convergence transfers this pairing to a sufficiently large finite momentum cutoff, but not the uncut pointwise support separation.

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