The μ differentiation experiment (Entry 9) showed that continuous adaptation
destroys gradient structure: ε=0.03 every step causes μ to overshoot, boundary zone thins and disappears,
and the organism homogenizes. The homeostatic pull (0.001) was 30× weaker than the adaptation rate.
Core hypothesis: If adaptation is pulsed (episodic) rather than continuous,
the flow field has time to re-establish spatial structure between adaptation events.
Stronger homeostasis can pull μ back toward baseline, preventing the overshoot.
Experiment: 12 runs spanning a parametric grid of homeostatic strength
{0, 0.001, 0.003, 0.01, 0.03, 0.10} × adaptation interval {1, 10, 50, 75, 100, 125, 150, 200}.
3000 steps per run, snapshots every 50 steps. Extended the best config to 4500 steps.
| hs | ai | Final Δμ | Boundary? | Outcome |
| 0 | 1 | — | dies ~600 | No adaptation: boundary death still occurs |
| 0.001 | 1 | — | dies ~600 | Original behavior: continuous, weak homeo |
| 0.001 | 100 | — | dies ~2400 | Sparsity delays collapse but doesn't prevent |
| 0.01 | 1 | — | dies ~1200 | 10× homeo helps but continuous adaptation still kills |
| 0.01 | 100 | 0.222 | ALIVE | ★ Sweet spot — gradient preserved, stable Δμ |
| 0.01 | 50 | — | dies ~2400 | Too frequent — doesn't give flow time to recover |
| 0.01 | 75 | — | dies ~2700 | Close but overshoots eventually |
| 0.01 | 125 | — | dies ~2400 | Longer interval loses homeostatic grip |
| 0.01 | 150 | 0.062 | ALIVE | Δμ smaller, gradient narrowing |
| 0.01 | 200 | 0.054 | ALIVE | Very weak differentiation, n_gradient shrinking |
| 0.03 | 100 | — | dies ~2400 | Stronger homeo can't compensate at this interval |
| 0.10 | 100 | — | dies ~2400 | Very strong homeo: μ barely moves, structure still collapses |
Key finding — sweet spot at hs=0.01, ai=100: This is the only configuration
where the boundary zone survives to 3000 steps with a genuine Δμ signal. μ_interior stabilizes
around 0.45-0.52 while μ_boundary stays at 0.30-0.42. The n gradient (interior−boundary local density)
is preserved at ~0.40-0.49.
But it's still precarious: At t~2700, the trajectory bifurcates — Δμ jumps from ~0.08
to ~0.22 as a late-stage adaptation event pushes interior μ up. Extended to 4500 steps, the boundary
eventually disappears (~3600+). The sweet spot buys time but isn't a permanent equilibrium.
Insight — temporal structure matters: The relationship between adaptation
timescale and homeostatic strength is a new control dimension. Continuous adaptation (ai=1)
always kills spatial structure regardless of homeostatic strength — the flow field needs
time to re-establish the gradient. There's a narrow window where adaptation pulses are
spaced far enough (≥100 steps) to allow recovery but not so far (≥150) that μ differentiation
fades. The product hs·ai may be the controlling parameter.
Assessment: We've established that episodic adaptation with calibrated
homeostasis can maintain spatial structure for extended periods while still producing
parameter differentiation. The next step is to test whether this regime can be made
stable — a true equilibrium where the gradient self-maintains rather than
eventually collapsing. Candidates: adaptive homeostatic strength, saturating adaptation
(μ_max), or feedback from the gradient width itself.