← CPL / 05 · First Reproduction of the Small-N Toy LP
The first independent reproduction of the bandwidth-one adversarial-law mechanism — the document states up front that this is not a reproduction of Anthropic's $N=256$ exact-rational LP, and positions are restricted to a discrete circular grid. For an explicit mixture with $N=4,M=24$, the mixed result gives $\bar S(1)=1/4,\bar S(2)=1/2,\bar S(3)=3/4$ (an exact match to the open-band CUE target), yet $\bar p=70.18\%$ — already reproducing, in a toy class far narrower than the official one, the phenomenon that “open-band pair rows matching CUE exactly ⇏ simple fraction near 1.” The same solution also makes the constrained $j<N$ rows fit CUE almost perfectly, while producing a huge spike at the unobserved boundary row ($j=256$) ($S(256)\approx211.43$, consistent with the official kernel-checked bound $|D(1)|\le0.82395317$) — this is defined as the Boundary-Spike Obstruction (BSO). The document then runs two sets of experiments to test how actionable this mechanism is: adding just one boundary constraint $\mathbb E[S(N)]\le B$ pushes the adversarial floor all the way from 70.18% (unconstrained) to 81.91% ($B=1.0$); a support-extension experiment points in the same direction, but the document explicitly warns that these percentages should not be matched one-to-one against Claude's real support thresholds $1.04,1.26,1.70$ — the toy grid is too narrow and the row sampling too coarse.
Relationship to other documents, stated as far as possible in the document's own words, not my interpretation.
“When only the open-band pair-correlation observables are fixed, a low-simple-fraction configuration law can shift most of the information that distinguishes multiplicity/collision structure out to the unobserved band at α≈1 or beyond.” — from this document's definition of “7. Boundary-Spike Obstruction (BSO).”
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