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A new theoretical framework combines differential heterogenesis with autopoiesis to explain how living systems can develop historicity and maintain themselves. The framework uses heterogeneous operator assemblages that obey two closure constraints: a fixed–point condition that keeps the interface stable, and a reproduction condition that preserves the operator composition across divisions. In a concrete example, the Gray–Scott reaction–diffusion equation is used outside a free surface while an anisotropic, gradient‑dependent diffusion operator is used inside. Numerical simulations show that this heterogenetic assembly produces hexagonal cells that retain their shape after each division and fill the domain until the substrate is exhausted. In contrast, a homogeneous Gray–Scott model with identical operators on both sides of the interface generates round cells that lose their shape when multiplied.
| Already given by differential heterogenesis | Constraint added here | What the constraint yields |
|---|---|---|
| Spatial assemblage of heterogeneous operators composed over a domain | Fixed-point condition 𝒜(ϕ)=ϕ, hence 𝒜(Γ)=Γ | the assemblage persists as a solution of its own production, and the form it generates is self-maintaining rather than transient |
| Temporal assemblage of operators superposed and modulated in time | Reproduction condition C𝒜τ(𝒜)=𝒜 | the assemblage is reproduced with variation, since the whole stratification of operators is transmitted, so the form generated is inherited rather than re-invented |






The model’s construction relies on a free‑boundary multiphase system. The invariant interface γ satisfies γ\mathcal{A}_{ au}(ϕ)=ϕ, which follows from a Schauder‑type argument showing that a nonlinear, non‑local operator maps a closed bounded convex set into a compact subset of itself. The numerical evidence, however, is the only way to confirm the two closure conditions for this heterogeneous system; analytical existence and stability proofs are not yet available.
These results illustrate how changing the local operator across a moving interface can break rotational symmetry and impose a preferred geometry on the emerging structure, while still allowing for self‑maintaining, self‑reproducing dynamics governed by historical constraints.