← NS-FCBP / FCBP-04 · Moving-Filter Telescoping, Continuous Filter Drift, Horizon Alignment, Time-Thickness Barrier, and Borderline Critical Lift

v0.1 Cycle VI 2026-08-16

FCBP-04: Moving-Filter Telescoping, Continuous Filter Drift, Horizon Alignment, Time-Thickness Barrier, and Borderline Critical Lift

Moving-Filter Telescoping, Continuous Filter Drift, Horizon Alignment, Time-Thickness Barrier, and Borderline Critical Lift

FCBP-03 produces the first non-summable pressure–flux scale schedule (∑r_k²<∞ but ∑r_k/r_0=∞), proving a genuine "schedule lift" — but a schedule lift is not yet a "horizon critical lift." This round handles two compatibility problems: the filter must move with the physical scale, and the window slices must genuinely approach the singular horizon with the correct parabolic geometry. The first problem can largely be closed; the second reveals a new time-thickness barrier. Proves an L² filtering-scale derivative estimate for smooth compactly-supported mollifiers, deriving the exact coarse-grained Navier–Stokes equation for a continuous time-dependent filter; under slow schedules, the filter-drift work of a linearly moving relative filter is universally controlled by the Leray energy/dissipation budget — so a discrete filter-switch stack can be bypassed by continuous filter drift. However, proves a parabolic-alignment summability theorem: if adjacent full-thickness parabolic window slices accumulate at T* while staying within O(1) local parabolic age of the horizon, then ∑r_k must be finite — a non-summable slow schedule must therefore lose fixed parabolic horizon alignment. The second route uses horizon-aligned thin window slices, where a co-moving heat-semigroup filter can exactly absorb the filter drift, but the universal time-thickness theorem proved here shows that even when ∑w_k diverges, the bounded normalized power can still be summable.

Connections

Relationship to the rest of the series, stated as closely as possible in the document's own words, not my interpretation.

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