Arithmetic dynamics, evolutionary learning, and bioelectric morphogenesis all describe form as the destination of an iterated update on a structured state space. Joseph Silverman's dictionary sends torsion points to periodic and preperiodic points; Richard Watson's evolution-as-learning sends past selection to developmental attractors; Michael Levin's target morphology is a stored setpoint a tissue relaxes back toward. The common denominator is not form in a mystical sense, but the tractable fact that iterated systems can acquire privileged regions of state space that behave like memories, goals, or destinies.
The strong, defensible claim is shared dynamical structure. The leap from there to “biology downloads pre-existing Platonic forms” is a separate, speculative interpretation, and this playground keeps the two apart.
A tissue is a grid of cells with a continuous internal state. A low-rank associative memory pulls the field toward three orthonormalised stored morphologies, while local diffusion couples neighbours. With symmetric coupling the deterministic dynamics descend a Lyapunov energy:
Stored morphologies are the minima. A lesion pushes the state up a hill; if memory is above the retrieval threshold, the same memory rolls it back down and the form regenerates. The calibration panel measures that repair fidelity, and is honest about the rigid regime where a lesion leaves a frozen scar instead.
The sharpest caution is the one Silverman makes about his own field: there is a powerful dictionary, but “no precise dictionary.” An arithmetic periodic point is exact, discrete, and noise-free; a biological attractor is approximate, dissipative, history-sensitive, and only metastable. Turn up the noise slider and the basin shimmers: it was never a fixed point. The analogy is a source of structure and discipline, not a proof that the same object lives in both worlds.
This is a transparent sandbox for the shared attractor logic, not a validated regenerative simulator. It omits mechanics, gene regulation, and electrophysiology; the templates and weights are hand-chosen; and mainstream accounts (positional information, reaction-diffusion, mechanochemistry) already explain much of the same patterning without invoking stored memories. There is no clean deterministic parameter-to-scalar map for a live stochastic field, so there is no tornado chart here; the sweep and the calibration carry the quantitative weight instead.