Two points leave the origin at the same speed. A's triadic loop is shorter than B's
(11.5, 0.5) bus line, so each lap the slip T−D walks B's phase back;
B's bus line runs through the prime mask, so it dwells there and is caught repeatedly — the
resonant reading of the corrected geometry.
Each run computes the figure-2 outcome for these parameters server-side — via the same generator that defines the figure — and records one row to the dataset.
Every recorded run (oxexp-slip · local-first).
| seq | mask | yellow | laps | T | D | slip | beat | catches | 1st |
|---|
The catch laps laid onto the 4×21 grid (the NodeMatrix), mask (2,0,3,1).
Over 84 laps = one matrix the slip lights 8 cells in two clusters — a clean
4-per-2×21 phase-lock.
Literal: 4 catches per 2×21 — clean to ~cycle 13, then
the beat (45.28) drifts off 2×21. Interpretive: the slip phase-locks to the 21-cycle
(FIGURE-2's "21-Cycle Phase-Lock Compression", measured); 4×21 = 84 is the coherence
window where the readout is integer-clean — an independent route landing on the substrate's NodeMatrix.
Two modes of how linearity advances. This view reads the same slip a second way; it does not generate or alter any record.
N = (N−1) + 1A single linearity adds one drifting unit at a time (O + C,
pro-causal). It self-certifies its 1, so it slips — deterministic only to
110, then 22 bits of bifurcation, then rupture at 132.
5 → 8 → 13Two linearities lock each other (+ E, the anti-causal return): the
increment is the grounded past, ratio φ, the 5 open to ground left or
right. The mode that advances past the rupture — the non-linear free zone.