← NS_O / 10 / C3-H: Ancestry Renormalization, the Unit-Shell Anchor, and the Critical Compactness Barrier
C3-G established a conditional causal genealogy under explicit assumptions. This round applies a viscosity-normalized critical rescaling to that genealogy, $v_n(y,s)=\nu^{-1}\lambda_n^{-1}u(x_n+y/\lambda_n,t_n+s/(\nu\lambda_n^2))$, and asks whether this directly yields a nontrivial ancient critical element to which existing backward-uniqueness/rigidity theorems can be applied. The verdict is explicit: not directly. Because of the first-crossing definition, the rescaled field retains a Persistent First-Crossing Trace (Theorem 5.1): for $s<0$ the unit-shell amplitude is strictly below the threshold, and at $s=0$ it exactly equals the threshold — a pure consequence of the scaling. Using a uniform Bernstein derivative bound plus an Arzelà–Ascoli diagonal extraction, it proves Unit-Shell Snapshot Compactness (Theorem 9.1): a nonzero, smooth, band-limited limit profile $w_\ast$ exists, satisfying the helical eigen-relation and carrying genuinely nonzero local critical mass. The backward lifespan extends to $(-\infty,0]$ because $\nu\lambda_n^2t_n\to\infty$. However, the document cites the external Seregin theorem (potential blow-up requires $\|u(t)\|_3\to\infty$, not merely $\limsup$) together with critical scale invariance to prove Renormalized global critical-norm divergence (Theorem 13.1): $\|v_n(0)\|_3\to\infty$, with the $\dot H^{1/2}$ norm likewise diverging — this is precisely the Critical Compactness Barrier (Theorem 15.1): the unit-shell anchor is compact, but the full rescaled field is unbounded in both $L^3$ and $\dot H^{1/2}$, so the Kenig–Koch or Gallagher–Koch–Planchon compactness/profile-decomposition theorems — which require a bounded critical sequence — cannot be applied directly. The document explicitly notes that amplitude normalization (dividing by the $L^3$ norm) is also not a legal N–S renormalization, since doing so would rewrite the equation itself. The remaining divergent part must be explicitly preserved as a critical background defect, not silently discarded (echoing the non-collapsing spirit of the X-Integration). A second no-go appears in the rescaling of the causal edge: the normalized time gap $\delta_n=\nu\lambda_n^2(t_n^c-t_n^p)$ is only known to satisfy $0<\delta_n\le\theta$, with no uniform positive lower bound, so $\delta_n\to0$ remains entirely possible — legality at every scale does not imply legality in the limit, and strict causality is not a property preserved under renormalization. The document closes with a Renormalization Trichotomy: Branch A (fully compact, but already proved impossible as a bounded global $L^3$ object), Branch B (background defect, requiring classification of where the divergence goes), and Branch C (causal collapse, requiring activation depth rather than physical time as the ordering parameter).
Relationship to the rest of the series, stated as closely as possible in the document's own words, not my interpretation.
“Legal at every scale ⟹̸ legal in the limit. This is exactly one of the X-Integration's most important limit guards.” — quoted from the paper's Section 43.
Loading…