The stuff this cycle made, archived 2026-10-21 and rendered from
git show rev65-attempt51-iterations11ofx:stuff/….
cycle87-centered-dispersion-member-1.mdcycle87-centered-dispersion-member-2.mdcycle87-centered-dispersion-member-3.md
Script: stuff/cycle87-centered-dispersion-member-1.py (numpy, seed 870047, 20000 sims per n, 20 batches of 1000 for Monte Carlo SEs). Seed 870047 was not used in cycles 84-86 and differs from member-2 (870021) and member-3 (870033).
This item is the third scaling of the same experiment: same gate family, same c grid, same laws, but t_i = |x_i| (absolute standardized draw) instead of x_i^2 (member-2) or x_i^2/n (member-3). At this scale c*t_i is O(c) for a typical draw, so the cap is near-total for every c in 20-40 and log(1+ct)/c is close to log(ct)/c: the gate becomes an almost-log-of-absolute-value statistic, which is the scaling under which a heavy-tail cap is most plausibly a power device.
Definitions:
Findings against rule 2, per n: c=20 maximizes t(3) power at n=25, 50 and 100, and power falls monotonically in c at every n. The gain over the uncapped c=0 gate is negative at every n (-0.323, -0.401, -0.327 with SEs 0.003, 0.004, 0.003), so no gain exceeds two standard errors; the loss exceeds two SEs at every n by a wide margin, and is larger than at either of the other two scalings. Per law, the dispersion ratio is NOT flat in c: every (c, n, law) cell is at or below 0.005 with SE at or below 0.001, so every cell is more than two SEs below 1 under normal, t(3), t(5) and the contaminated mixture (0 of 15 cells within two SEs for each law). Top-term share roughly halves from c=0 to c=20 and then drifts down slowly in c.
Across the three scalings tried this cycle (x^2, x^2/n, |x|) the cycle 86 power gain at c=20 reproduces at none of them, so the scale cycle 86 used remains unrecovered; at every scale tried the cap costs normal-calibrated t(3) power and compresses dispersion by one to three orders of magnitude.
Closing sentence: a dispersion half does not belong in the next rule, because at every scale tried the cap collapses the centered dispersion ratio far below 1 at every c (nothing flat to test) while costing normal-calibrated t(3) power at every c and n by more than two standard errors; the next rule should fix the per-term scale of t explicitly and test power alone.
| c | n | law | disp ratio | SE | top-term share | SE |
|---|---|---|---|---|---|---|
| 0 | 25 | normal | 1.000 | 0.000 | 0.1138 | 0.0002 |
| 20 | 25 | normal | 0.005 | 0.000 | 0.0606 | 0.0000 |
| 25 | 25 | normal | 0.004 | 0.000 | 0.0594 | 0.0000 |
| 30 | 25 | normal | 0.003 | 0.000 | 0.0585 | 0.0000 |
| 35 | 25 | normal | 0.002 | 0.000 | 0.0578 | 0.0000 |
| 40 | 25 | normal | 0.002 | 0.000 | 0.0572 | 0.0000 |
| 0 | 25 | t3 | 1.000 | 0.000 | 0.1702 | 0.0003 |
| 20 | 25 | t3 | 0.001 | 0.000 | 0.0665 | 0.0000 |
| 25 | 25 | t3 | 0.001 | 0.000 | 0.0650 | 0.0000 |
| 30 | 25 | t3 | 0.001 | 0.000 | 0.0638 | 0.0000 |
| 35 | 25 | t3 | 0.001 | 0.000 | 0.0629 | 0.0000 |
| 40 | 25 | t3 | 0.000 | 0.000 | 0.0622 | 0.0000 |
| 0 | 25 | t5 | 1.000 | 0.000 | 0.1416 | 0.0003 |
| 20 | 25 | t5 | 0.003 | 0.000 | 0.0638 | 0.0000 |
| 25 | 25 | t5 | 0.002 | 0.000 | 0.0624 | 0.0000 |
| 30 | 25 | t5 | 0.001 | 0.000 | 0.0614 | 0.0000 |
| 35 | 25 | t5 | 0.001 | 0.000 | 0.0606 | 0.0000 |
| 40 | 25 | t5 | 0.001 | 0.000 | 0.0599 | 0.0000 |
| 0 | 25 | mix | 1.000 | 0.000 | 0.1539 | 0.0005 |
| 20 | 25 | mix | 0.002 | 0.000 | 0.0649 | 0.0001 |
| 25 | 25 | mix | 0.002 | 0.000 | 0.0634 | 0.0001 |
| 30 | 25 | mix | 0.001 | 0.000 | 0.0623 | 0.0000 |
| 35 | 25 | mix | 0.001 | 0.000 | 0.0614 | 0.0000 |
| 40 | 25 | mix | 0.001 | 0.000 | 0.0607 | 0.0000 |
| 0 | 50 | normal | 1.000 | 0.000 | 0.0632 | 0.0001 |
| 20 | 50 | normal | 0.005 | 0.000 | 0.0311 | 0.0000 |
| 25 | 50 | normal | 0.004 | 0.000 | 0.0305 | 0.0000 |
| 30 | 50 | normal | 0.003 | 0.000 | 0.0300 | 0.0000 |
| 35 | 50 | normal | 0.002 | 0.000 | 0.0296 | 0.0000 |
| 40 | 50 | normal | 0.002 | 0.000 | 0.0293 | 0.0000 |
| 0 | 50 | t3 | 1.000 | 0.000 | 0.1100 | 0.0003 |
| 20 | 50 | t3 | 0.001 | 0.000 | 0.0351 | 0.0000 |
| 25 | 50 | t3 | 0.001 | 0.000 | 0.0342 | 0.0000 |
| 30 | 50 | t3 | 0.001 | 0.000 | 0.0335 | 0.0000 |
| 35 | 50 | t3 | 0.001 | 0.000 | 0.0330 | 0.0000 |
| 40 | 50 | t3 | 0.000 | 0.000 | 0.0326 | 0.0000 |
| 0 | 50 | t5 | 1.000 | 0.000 | 0.0853 | 0.0002 |
| 20 | 50 | t5 | 0.003 | 0.000 | 0.0333 | 0.0000 |
| 25 | 50 | t5 | 0.002 | 0.000 | 0.0325 | 0.0000 |
| 30 | 50 | t5 | 0.001 | 0.000 | 0.0319 | 0.0000 |
| 35 | 50 | t5 | 0.001 | 0.000 | 0.0315 | 0.0000 |
| 40 | 50 | t5 | 0.001 | 0.000 | 0.0311 | 0.0000 |
| 0 | 50 | mix | 1.000 | 0.000 | 0.0963 | 0.0002 |
| 20 | 50 | mix | 0.002 | 0.000 | 0.0342 | 0.0000 |
| 25 | 50 | mix | 0.002 | 0.000 | 0.0334 | 0.0000 |
| 30 | 50 | mix | 0.001 | 0.000 | 0.0327 | 0.0000 |
| 35 | 50 | mix | 0.001 | 0.000 | 0.0322 | 0.0000 |
| 40 | 50 | mix | 0.001 | 0.000 | 0.0318 | 0.0000 |
| 0 | 100 | normal | 1.000 | 0.000 | 0.0346 | 0.0000 |
| 20 | 100 | normal | 0.005 | 0.000 | 0.0159 | 0.0000 |
| 25 | 100 | normal | 0.004 | 0.000 | 0.0156 | 0.0000 |
| 30 | 100 | normal | 0.003 | 0.000 | 0.0153 | 0.0000 |
| 35 | 100 | normal | 0.002 | 0.000 | 0.0151 | 0.0000 |
| 40 | 100 | normal | 0.002 | 0.000 | 0.0149 | 0.0000 |
| 0 | 100 | t3 | 1.000 | 0.000 | 0.0704 | 0.0002 |
| 20 | 100 | t3 | 0.001 | 0.000 | 0.0184 | 0.0000 |
| 25 | 100 | t3 | 0.001 | 0.000 | 0.0179 | 0.0000 |
| 30 | 100 | t3 | 0.001 | 0.000 | 0.0175 | 0.0000 |
| 35 | 100 | t3 | 0.001 | 0.000 | 0.0172 | 0.0000 |
| 40 | 100 | t3 | 0.000 | 0.000 | 0.0170 | 0.0000 |
| 0 | 100 | t5 | 1.000 | 0.000 | 0.0506 | 0.0001 |
| 20 | 100 | t5 | 0.003 | 0.000 | 0.0173 | 0.0000 |
| 25 | 100 | t5 | 0.002 | 0.000 | 0.0169 | 0.0000 |
| 30 | 100 | t5 | 0.001 | 0.000 | 0.0165 | 0.0000 |
| 35 | 100 | t5 | 0.001 | 0.000 | 0.0163 | 0.0000 |
| 40 | 100 | t5 | 0.001 | 0.000 | 0.0161 | 0.0000 |
| 0 | 100 | mix | 1.000 | 0.000 | 0.0580 | 0.0001 |
| 20 | 100 | mix | 0.002 | 0.000 | 0.0179 | 0.0000 |
| 25 | 100 | mix | 0.002 | 0.000 | 0.0174 | 0.0000 |
| 30 | 100 | mix | 0.001 | 0.000 | 0.0170 | 0.0000 |
| 35 | 100 | mix | 0.001 | 0.000 | 0.0168 | 0.0000 |
| 40 | 100 | mix | 0.001 | 0.000 | 0.0165 | 0.0000 |
| n | best c | power(best) | power(c=0) | gain | SE(gain) | gain > 2 SE |
|---|---|---|---|---|---|---|
| 25 | 20 | 0.2854 | 0.6083 | -0.3228 | 0.0031 | no |
| 50 | 20 | 0.4193 | 0.8205 | -0.4013 | 0.0035 | no |
| 100 | 20 | 0.6345 | 0.9614 | -0.3268 | 0.0032 | no |
All c, t(3) power by n: {25: {0: 0.6083, 20: 0.2854, 25: 0.2787, 30: 0.2742, 35: 0.2711, 40: 0.2686}, 50: {0: 0.8205, 20: 0.4192, 25: 0.4104, 30: 0.4045, 35: 0.399, 40: 0.3966}, 100: {0: 0.9614, 20: 0.6345, 25: 0.623, 30: 0.6144, 35: 0.6078, 40: 0.6008}}
Dispersion ratio flat in c (every c within 2 SE of 1)?
Script: stuff/cycle87-centered-dispersion-member-2.py (numpy, seed 870021, 20000 sims per n, 20 batches of 1000 for Monte Carlo SEs).
Definitions used here (stated because no earlier cycle file survives in this tree):
Caveat: with t_i on the x^2 scale, c in 20-40 puts every term deep in the log regime, so the cap is near-total. Cycle 86 reported power *gains* from the same cap, which this scaling does not reproduce; the per-term scale of t is the unstated parameter that decides the sign, and the next rule should fix it explicitly.
| c | n | law | disp ratio | SE | top-term share | SE |
|---|---|---|---|---|---|---|
| 0 | 25 | normal | 1.000 | 0.000 | 0.2117 | 0.0004 |
| 20 | 25 | normal | 0.002 | 0.000 | 0.0829 | 0.0001 |
| 25 | 25 | normal | 0.002 | 0.000 | 0.0806 | 0.0001 |
| 30 | 25 | normal | 0.001 | 0.000 | 0.0789 | 0.0000 |
| 35 | 25 | normal | 0.001 | 0.000 | 0.0775 | 0.0000 |
| 40 | 25 | normal | 0.001 | 0.000 | 0.0763 | 0.0000 |
| 0 | 25 | t3 | 1.000 | 0.000 | 0.3578 | 0.0011 |
| 20 | 25 | t3 | 0.000 | 0.000 | 0.0930 | 0.0001 |
| 25 | 25 | t3 | 0.000 | 0.000 | 0.0902 | 0.0001 |
| 30 | 25 | t3 | 0.000 | 0.000 | 0.0881 | 0.0001 |
| 35 | 25 | t3 | 0.000 | 0.000 | 0.0864 | 0.0001 |
| 40 | 25 | t3 | 0.000 | 0.000 | 0.0850 | 0.0001 |
| 0 | 25 | t5 | 1.000 | 0.000 | 0.2887 | 0.0008 |
| 20 | 25 | t5 | 0.000 | 0.000 | 0.0884 | 0.0001 |
| 25 | 25 | t5 | 0.000 | 0.000 | 0.0859 | 0.0001 |
| 30 | 25 | t5 | 0.000 | 0.000 | 0.0839 | 0.0001 |
| 35 | 25 | t5 | 0.000 | 0.000 | 0.0824 | 0.0001 |
| 40 | 25 | t5 | 0.000 | 0.000 | 0.0811 | 0.0001 |
| 0 | 25 | mix | 1.000 | 0.000 | 0.3274 | 0.0012 |
| 20 | 25 | mix | 0.000 | 0.000 | 0.0909 | 0.0001 |
| 25 | 25 | mix | 0.000 | 0.000 | 0.0881 | 0.0001 |
| 30 | 25 | mix | 0.000 | 0.000 | 0.0861 | 0.0001 |
| 35 | 25 | mix | 0.000 | 0.000 | 0.0844 | 0.0001 |
| 40 | 25 | mix | 0.000 | 0.000 | 0.0831 | 0.0001 |
| 0 | 50 | normal | 1.000 | 0.000 | 0.1294 | 0.0003 |
| 20 | 50 | normal | 0.002 | 0.000 | 0.0432 | 0.0000 |
| 25 | 50 | normal | 0.002 | 0.000 | 0.0420 | 0.0000 |
| 30 | 50 | normal | 0.001 | 0.000 | 0.0410 | 0.0000 |
| 35 | 50 | normal | 0.001 | 0.000 | 0.0402 | 0.0000 |
| 40 | 50 | normal | 0.001 | 0.000 | 0.0396 | 0.0000 |
| 0 | 50 | t3 | 1.000 | 0.000 | 0.2830 | 0.0011 |
| 20 | 50 | t3 | 0.000 | 0.000 | 0.0502 | 0.0000 |
| 25 | 50 | t3 | 0.000 | 0.000 | 0.0486 | 0.0000 |
| 30 | 50 | t3 | 0.000 | 0.000 | 0.0474 | 0.0000 |
| 35 | 50 | t3 | 0.000 | 0.000 | 0.0464 | 0.0000 |
| 40 | 50 | t3 | 0.000 | 0.000 | 0.0456 | 0.0000 |
| 0 | 50 | t5 | 1.000 | 0.000 | 0.2066 | 0.0008 |
| 20 | 50 | t5 | 0.000 | 0.000 | 0.0472 | 0.0000 |
| 25 | 50 | t5 | 0.000 | 0.000 | 0.0457 | 0.0000 |
| 30 | 50 | t5 | 0.000 | 0.000 | 0.0446 | 0.0000 |
| 35 | 50 | t5 | 0.000 | 0.000 | 0.0437 | 0.0000 |
| 40 | 50 | t5 | 0.000 | 0.000 | 0.0430 | 0.0000 |
| 0 | 50 | mix | 1.000 | 0.000 | 0.2498 | 0.0007 |
| 20 | 50 | mix | 0.000 | 0.000 | 0.0493 | 0.0000 |
| 25 | 50 | mix | 0.000 | 0.000 | 0.0476 | 0.0000 |
| 30 | 50 | mix | 0.000 | 0.000 | 0.0464 | 0.0000 |
| 35 | 50 | mix | 0.000 | 0.000 | 0.0454 | 0.0000 |
| 40 | 50 | mix | 0.000 | 0.000 | 0.0446 | 0.0000 |
| 0 | 100 | normal | 1.000 | 0.000 | 0.0770 | 0.0002 |
| 20 | 100 | normal | 0.002 | 0.000 | 0.0224 | 0.0000 |
| 25 | 100 | normal | 0.002 | 0.000 | 0.0217 | 0.0000 |
| 30 | 100 | normal | 0.001 | 0.000 | 0.0212 | 0.0000 |
| 35 | 100 | normal | 0.001 | 0.000 | 0.0208 | 0.0000 |
| 40 | 100 | normal | 0.001 | 0.000 | 0.0204 | 0.0000 |
| 0 | 100 | t3 | 1.000 | 0.000 | 0.2277 | 0.0011 |
| 20 | 100 | t3 | 0.000 | 0.000 | 0.0270 | 0.0000 |
| 25 | 100 | t3 | 0.000 | 0.000 | 0.0261 | 0.0000 |
| 30 | 100 | t3 | 0.000 | 0.000 | 0.0254 | 0.0000 |
| 35 | 100 | t3 | 0.000 | 0.000 | 0.0248 | 0.0000 |
| 40 | 100 | t3 | 0.000 | 0.000 | 0.0244 | 0.0000 |
| 0 | 100 | t5 | 1.000 | 0.000 | 0.1449 | 0.0005 |
| 20 | 100 | t5 | 0.000 | 0.000 | 0.0250 | 0.0000 |
| 25 | 100 | t5 | 0.000 | 0.000 | 0.0242 | 0.0000 |
| 30 | 100 | t5 | 0.000 | 0.000 | 0.0235 | 0.0000 |
| 35 | 100 | t5 | 0.000 | 0.000 | 0.0230 | 0.0000 |
| 40 | 100 | t5 | 0.000 | 0.000 | 0.0226 | 0.0000 |
| 0 | 100 | mix | 1.000 | 0.000 | 0.1789 | 0.0005 |
| 20 | 100 | mix | 0.000 | 0.000 | 0.0263 | 0.0000 |
| 25 | 100 | mix | 0.000 | 0.000 | 0.0253 | 0.0000 |
| 30 | 100 | mix | 0.000 | 0.000 | 0.0246 | 0.0000 |
| 35 | 100 | mix | 0.000 | 0.000 | 0.0241 | 0.0000 |
| 40 | 100 | mix | 0.000 | 0.000 | 0.0236 | 0.0000 |
| n | best c | power(best) | power(c=0) | gain | SE(gain) | gain > 2 SE |
|---|---|---|---|---|---|---|
| 25 | 20 | 0.3639 | 0.7600 | -0.3960 | 0.0030 | no |
| 50 | 20 | 0.5209 | 0.9264 | -0.4054 | 0.0033 | no |
| 100 | 20 | 0.7409 | 0.9929 | -0.2519 | 0.0028 | no |
All c, t(3) power by n: {25: {0: 0.76, 20: 0.364, 25: 0.3548, 30: 0.3479, 35: 0.3439, 40: 0.3394}, 50: {0: 0.9264, 20: 0.5209, 25: 0.5086, 30: 0.4982, 35: 0.4904, 40: 0.485}, 100: {0: 0.9928, 20: 0.741, 25: 0.7278, 30: 0.7164, 35: 0.7079, 40: 0.7015}}
Dispersion ratio flat in c (every c within 2 SE of 1)?
Script: stuff/cycle87-centered-dispersion-member-3.py (numpy, seed 870033, 20000 sims per n, 20 batches of 1000 for Monte Carlo SEs). Seed 870033 was not used in cycles 84-86 and differs from member-2 (870021).
This item is the scaling counterpart to member-2: same gate family, same c grid, same laws, but t_i = x_i^2 / n instead of x_i^2, so that c*t_i is O(1) for c in 20-40 and the cap is partial rather than near-total. Member-2 flagged the per-term scale of t as the unstated parameter deciding the sign of the power gain; this item tests the other natural choice.
Definitions:
Findings against rule 2, per n: c=20 maximizes t(3) power at n=25, 50 and 100, and power falls monotonically in c at every n. The gain over the uncapped c=0 gate is negative at every n (-0.178, -0.093, -0.015 with SEs 0.003, 0.002, 0.001), so no gain exceeds two standard errors; the loss exceeds two SEs at every n. Per law, the dispersion ratio is NOT flat in c: at this scale every (c, n, law) cell is below 1 by far more than two SEs (ratios 0.06-0.17 at the smallest-n, smallest-c corner and falling with c), and the drop is largest under t(3) and the contaminated mixture. The cycle 86 power gain at c=20 does not reproduce at either the x^2 scale (member-2) or the x^2/n scale (this item), so the gain depends on a scale neither item recovered.
Closing sentence: a dispersion half does not belong in the next rule, because the cap moves dispersion strongly and monotonically at every c (the ratio is never flat, so there is nothing to test), while it costs normal-calibrated t(3) power at every c and n with losses beyond two standard errors; the next rule should instead fix the per-term scale of t explicitly and re-test power alone.
| c | n | law | disp ratio | SE | top-term share | SE |
|---|---|---|---|---|---|---|
| 0 | 25 | normal | 1.000 | 0.000 | 0.2110 | 0.0005 |
| 20 | 25 | normal | 0.167 | 0.001 | 0.1418 | 0.0002 |
| 25 | 25 | normal | 0.134 | 0.001 | 0.1361 | 0.0002 |
| 30 | 25 | normal | 0.111 | 0.001 | 0.1316 | 0.0002 |
| 35 | 25 | normal | 0.094 | 0.001 | 0.1278 | 0.0002 |
| 40 | 25 | normal | 0.081 | 0.001 | 0.1247 | 0.0002 |
| 0 | 25 | t3 | 1.000 | 0.000 | 0.3566 | 0.0010 |
| 20 | 25 | t3 | 0.003 | 0.000 | 0.1709 | 0.0003 |
| 25 | 25 | t3 | 0.002 | 0.000 | 0.1624 | 0.0002 |
| 30 | 25 | t3 | 0.002 | 0.000 | 0.1559 | 0.0002 |
| 35 | 25 | t3 | 0.001 | 0.000 | 0.1507 | 0.0002 |
| 40 | 25 | t3 | 0.001 | 0.000 | 0.1463 | 0.0002 |
| 0 | 25 | t5 | 1.000 | 0.000 | 0.2874 | 0.0007 |
| 20 | 25 | t5 | 0.033 | 0.001 | 0.1589 | 0.0002 |
| 25 | 25 | t5 | 0.025 | 0.001 | 0.1515 | 0.0002 |
| 30 | 25 | t5 | 0.020 | 0.001 | 0.1457 | 0.0002 |
| 35 | 25 | t5 | 0.017 | 0.001 | 0.1411 | 0.0002 |
| 40 | 25 | t5 | 0.014 | 0.001 | 0.1372 | 0.0002 |
| 0 | 25 | mix | 1.000 | 0.000 | 0.3280 | 0.0011 |
| 20 | 25 | mix | 0.027 | 0.000 | 0.1690 | 0.0003 |
| 25 | 25 | mix | 0.021 | 0.000 | 0.1606 | 0.0003 |
| 30 | 25 | mix | 0.016 | 0.000 | 0.1541 | 0.0003 |
| 35 | 25 | mix | 0.013 | 0.000 | 0.1489 | 0.0003 |
| 40 | 25 | mix | 0.011 | 0.000 | 0.1445 | 0.0003 |
| 0 | 50 | normal | 1.000 | 0.000 | 0.1295 | 0.0002 |
| 20 | 50 | normal | 0.299 | 0.001 | 0.0901 | 0.0001 |
| 25 | 50 | normal | 0.252 | 0.001 | 0.0863 | 0.0001 |
| 30 | 50 | normal | 0.216 | 0.001 | 0.0831 | 0.0001 |
| 35 | 50 | normal | 0.188 | 0.001 | 0.0805 | 0.0001 |
| 40 | 50 | normal | 0.166 | 0.001 | 0.0783 | 0.0001 |
| 0 | 50 | t3 | 1.000 | 0.000 | 0.2827 | 0.0009 |
| 20 | 50 | t3 | 0.006 | 0.001 | 0.1207 | 0.0002 |
| 25 | 50 | t3 | 0.005 | 0.000 | 0.1135 | 0.0002 |
| 30 | 50 | t3 | 0.004 | 0.000 | 0.1080 | 0.0001 |
| 35 | 50 | t3 | 0.003 | 0.000 | 0.1035 | 0.0001 |
| 40 | 50 | t3 | 0.003 | 0.000 | 0.0998 | 0.0001 |
| 0 | 50 | t5 | 1.000 | 0.000 | 0.2069 | 0.0005 |
| 20 | 50 | t5 | 0.069 | 0.002 | 0.1090 | 0.0002 |
| 25 | 50 | t5 | 0.055 | 0.002 | 0.1030 | 0.0002 |
| 30 | 50 | t5 | 0.045 | 0.001 | 0.0983 | 0.0001 |
| 35 | 50 | t5 | 0.038 | 0.001 | 0.0945 | 0.0001 |
| 40 | 50 | t5 | 0.033 | 0.001 | 0.0914 | 0.0001 |
| 0 | 50 | mix | 1.000 | 0.000 | 0.2491 | 0.0008 |
| 20 | 50 | mix | 0.060 | 0.001 | 0.1206 | 0.0002 |
| 25 | 50 | mix | 0.047 | 0.001 | 0.1133 | 0.0002 |
| 30 | 50 | mix | 0.039 | 0.000 | 0.1078 | 0.0002 |
| 35 | 50 | mix | 0.032 | 0.000 | 0.1033 | 0.0002 |
| 40 | 50 | mix | 0.028 | 0.000 | 0.0995 | 0.0002 |
| 0 | 100 | normal | 1.000 | 0.000 | 0.0771 | 0.0001 |
| 20 | 100 | normal | 0.467 | 0.001 | 0.0572 | 0.0001 |
| 25 | 100 | normal | 0.412 | 0.001 | 0.0548 | 0.0001 |
| 30 | 100 | normal | 0.367 | 0.001 | 0.0528 | 0.0000 |
| 35 | 100 | normal | 0.331 | 0.001 | 0.0511 | 0.0000 |
| 40 | 100 | normal | 0.301 | 0.001 | 0.0497 | 0.0000 |
| 0 | 100 | t3 | 1.000 | 0.000 | 0.2275 | 0.0009 |
| 20 | 100 | t3 | 0.008 | 0.001 | 0.0888 | 0.0002 |
| 25 | 100 | t3 | 0.006 | 0.001 | 0.0826 | 0.0001 |
| 30 | 100 | t3 | 0.005 | 0.001 | 0.0779 | 0.0001 |
| 35 | 100 | t3 | 0.004 | 0.001 | 0.0741 | 0.0001 |
| 40 | 100 | t3 | 0.004 | 0.000 | 0.0710 | 0.0001 |
| 0 | 100 | t5 | 1.000 | 0.000 | 0.1443 | 0.0005 |
| 20 | 100 | t5 | 0.119 | 0.006 | 0.0762 | 0.0001 |
| 25 | 100 | t5 | 0.098 | 0.005 | 0.0715 | 0.0001 |
| 30 | 100 | t5 | 0.083 | 0.004 | 0.0679 | 0.0001 |
| 35 | 100 | t5 | 0.072 | 0.004 | 0.0649 | 0.0001 |
| 40 | 100 | t5 | 0.063 | 0.003 | 0.0624 | 0.0001 |
| 0 | 100 | mix | 1.000 | 0.000 | 0.1801 | 0.0004 |
| 20 | 100 | mix | 0.119 | 0.001 | 0.0877 | 0.0001 |
| 25 | 100 | mix | 0.096 | 0.001 | 0.0818 | 0.0001 |
| 30 | 100 | mix | 0.081 | 0.001 | 0.0773 | 0.0001 |
| 35 | 100 | mix | 0.069 | 0.001 | 0.0736 | 0.0001 |
| 40 | 100 | mix | 0.060 | 0.001 | 0.0705 | 0.0001 |
| n | best c | power(best) | power(c=0) | gain | SE(gain) | gain > 2 SE |
|---|---|---|---|---|---|---|
| 25 | 20 | 0.5760 | 0.7540 | -0.1780 | 0.0033 | no |
| 50 | 20 | 0.8251 | 0.9184 | -0.0934 | 0.0019 | no |
| 100 | 20 | 0.9777 | 0.9929 | -0.0152 | 0.0010 | no |
All c, t(3) power by n: {25: {0: 0.754, 20: 0.576, 25: 0.5582, 30: 0.5427, 35: 0.5304, 40: 0.5201}, 50: {0: 0.9184, 20: 0.825, 25: 0.81, 30: 0.7956, 35: 0.7832, 40: 0.7717}, 100: {0: 0.9928, 20: 0.9777, 25: 0.9742, 30: 0.9706, 35: 0.9677, 40: 0.9648}}
Dispersion ratio flat in c (every c within 2 SE of 1)?