Check 1 of the pilot review: the timing gap between groups A and B over time (run 2026-10-14 14:47 Halifax). After the fact and exploratory: a description of the pilot's saved results, not a reading fixed in plan.md and not a new experiment. No model was run. A toy model: structure inside the model, not evidence about cells. Histories, not memory: differences are between intervention histories and the states they leave. Read: the pilot's 120 moment files (starts 103 to 114), each matching the hash in pilot_results.json. The gap reproduces the report's |A-B timing| at R (largest difference 1.6e-15 rad). Gap: |psi_A - psi_B| in radians; 0 means the two groups' rhythms are in step, about 1.571 (pi/2) is what unrelated rhythms average. Split: half of (lowered gap minus raised gap); positive means the raised arm's groups sit closer in timing. Error bars and 'clear' (more than 3 bars) as in the report. Answer: lasts. The medium (all 120 moments) split at R: +0.4114 +- 0.0339 (+12.1 bars; 12 of 12 starts above zero) split over (R+200, R+500]: +0.2571 +- 0.0155 (+16.6 bars; 12 of 12 starts above zero) share of the split at R still there over (R+200, R+500]: +0.625 +- 0.074 raised minus untouched: at R -0.4209 +- 0.0546 (-7.7 bars; 0 of 12 starts above zero) over (R+200, R+500] -0.2952 +- 0.0205 (-14.4 bars; 0 of 12 starts above zero) lowered minus untouched: at R +0.4018 +- 0.0448 (+9.0 bars; 12 of 12 starts above zero) over (R+200, R+500] +0.2189 +- 0.0365 (+6.0 bars; 12 of 12 starts above zero) common part: at R -0.0095 +- 0.0367 (-0.3 bars; 6 of 12 starts above zero) over (R+200, R+500] -0.0381 +- 0.0253 (-1.5 bars; 4 of 12 starts above zero) Pushes and shams (moments with both pushes built) push split: at R -0.0009 +- 0.0011 (-0.8 bars; 4 of 12 starts above zero) over (R+200, R+500] +0.1904 +- 0.0199 (+9.6 bars; 12 of 12 starts above zero) sham split: at R +0.0015 +- 0.0014 (+1.0 bars; 5 of 12 starts above zero) over (R+200, R+500] +0.0177 +- 0.0119 (+1.5 bars; 8 of 12 starts above zero) Medium against matched push, like for like (split difference) at R: +0.4071 +- 0.0350 (+11.6 bars; 12 of 12 starts above zero) over (R+200, R+500]: +0.0647 +- 0.0149 (+4.4 bars; 11 of 12 starts above zero) The medium's split by 100-unit block (from T; R = T+200) (T, T+100]: +0.1230 +- 0.0040 (+30.6 bars; 12 of 12 starts above zero) (T+100, R]: +0.3304 +- 0.0097 (+34.2 bars; 12 of 12 starts above zero) (R+0, R+100]: +0.3794 +- 0.0102 (+37.3 bars; 12 of 12 starts above zero) (R+100, R+200]: +0.3432 +- 0.0148 (+23.1 bars; 12 of 12 starts above zero) (R+200, R+300]: +0.3066 +- 0.0163 (+18.8 bars; 12 of 12 starts above zero) (R+300, R+400]: +0.2524 +- 0.0168 (+15.0 bars; 12 of 12 starts above zero) (R+400, R+500]: +0.2122 +- 0.0182 (+11.7 bars; 12 of 12 starts above zero) blocks with a clear positive split: (T, T+100], (T+100, R], (R+0, R+100], (R+100, R+200], (R+200, R+300], (R+300, R+400], (R+400, R+500] The medium's common part by block (from T) (T, T+100]: +0.0011 +- 0.0020 (+0.5 bars; 7 of 12 starts above zero) (T+100, R]: -0.0064 +- 0.0125 (-0.5 bars; 4 of 12 starts above zero) (R+0, R+100]: -0.0160 +- 0.0157 (-1.0 bars; 4 of 12 starts above zero) (R+100, R+200]: -0.0286 +- 0.0165 (-1.7 bars; 3 of 12 starts above zero) (R+200, R+300]: -0.0459 +- 0.0219 (-2.1 bars; 4 of 12 starts above zero) (R+300, R+400]: -0.0304 +- 0.0295 (-1.0 bars; 5 of 12 starts above zero) (R+400, R+500]: -0.0381 +- 0.0307 (-1.2 bars; 5 of 12 starts above zero) Push split, sham split and medium-minus-push split difference by block (from R) (R+0, R+100]: push +0.2663 +- 0.0095 (+28.0 bars; 12 of 12 starts above zero); sham +0.0057 +- 0.0045 (+1.3 bars; 8 of 12 starts above zero); difference +0.1109 +- 0.0108 (+10.3 bars; 12 of 12 starts above zero) (R+100, R+200]: push +0.2358 +- 0.0198 (+11.9 bars; 12 of 12 starts above zero); sham +0.0157 +- 0.0096 (+1.6 bars; 7 of 12 starts above zero); difference +0.1054 +- 0.0199 (+5.3 bars; 11 of 12 starts above zero) (R+200, R+300]: push +0.2127 +- 0.0217 (+9.8 bars; 12 of 12 starts above zero); sham +0.0267 +- 0.0124 (+2.2 bars; 10 of 12 starts above zero); difference +0.0916 +- 0.0156 (+5.9 bars; 12 of 12 starts above zero) (R+300, R+400]: push +0.1883 +- 0.0212 (+8.9 bars; 12 of 12 starts above zero); sham +0.0120 +- 0.0139 (+0.9 bars; 7 of 12 starts above zero); difference +0.0616 +- 0.0170 (+3.6 bars; 9 of 12 starts above zero) (R+400, R+500]: push +0.1701 +- 0.0226 (+7.5 bars; 12 of 12 starts above zero); sham +0.0145 +- 0.0210 (+0.7 bars; 7 of 12 starts above zero); difference +0.0408 +- 0.0228 (+1.8 bars; 8 of 12 starts above zero) Average gap by block (radians; untouched and medium from T, pushes and shams from R) untouched: 0.8077 0.8216 0.7947 0.8064 0.8252 0.7996 0.8118 medium raised: 0.6858 0.4848 0.3993 0.4345 0.4728 0.5168 0.5615 medium lowered: 0.9317 1.1456 1.1581 1.1209 1.0860 1.0216 0.9859 push raised: 0.5138 0.5323 0.5581 0.5737 0.6058 push lowered: 1.0465 1.0038 0.9836 0.9503 0.9460 sham raised: 0.7840 0.7649 0.7499 0.7676 0.7318 sham lowered: 0.7953 0.7962 0.8033 0.7915 0.7608 Limits Lower coherence makes each group's rhythm noisier, which pulls the average gap toward about 1.571. The lowered arm stays less coherent after R, so part of its wider gap can come from that. The matched push, at nearly the same coherence, is the comparison that separates timing from coherence level. Whether the gap carries the later-growth difference is not tested here; this only says whether it is still there when that difference appears. Compute: 27.9 seconds, in the foreground.