Construction 1: reciprocal production holding a coupling (A9, A10)

ċ₁ = 3c₂²/(1 + c₂²) − (1 + d₁(t))c₁, ċ₂ = 3c₁²/(1 + c₁²) − (1 + d₂(t))c₂.

  • Equilibria at d = 0. Symmetric equilibria solve c = 3c²/(1 + c²): 0, (3 − √5)/2 ≈ 0.382 (a saddle) and (3 + √5)/2 ≈ 2.618 (stable, eigenvalues −0.7454 and −1.2546). Since production is increasing there are no asymmetric equilibria. Resetting c₁ to 0 with c₂ at 2.618 recovers to (2.618, 2.618).
  • Invariance. For 0 ≤ dᵢ(t) ≤ 0.4 the box [1, 4]² is positively invariant: at c = 1 the inflow is at least 3/2 − 1.4 = 0.1, and at c = 4 the outflow is at least 4 − 48/17. A constant d = 0.4 settles at 1.456.
  • Fold. With constant d, positive equilibria exist iff 9 − 4(1 + d)² ≥ 0, that is d ≤ 0.5, and they merge at c = 1. Above it, 3M²/(1 + M²) ≤ 1.5M gives extinction from every start. A seed of 0.2 collapses and one of 0.5 grows. A10’s chart had three wrong points, which A10 corrected: (0.437, 2.291) at d = 0.1, (0.578, 1.729) at 0.3, (0.770, 1.299) at 0.45.
  • Coupling. Three units x with ẋ = −L(c)x, L = Bᵀ diag(a₁, a₂) B, aᵢ = max{cᵢ − ½, 0}. While c stays in [1, 4]², λ₂(L) ≥ 0.5, so the units synchronize at rate at least ½. A pulse ε on the first unit gives ẋ₃(0) = 0 and ẍ₃(0) = a₁a₂ε: the third unit responds at second order, through the second.
  • Knockout. Removing the c₂ → c₁ production collapses both capacities and with them the coupling, as CLAIM-516 requires.
  • Provenance. An outside controller supplying the same production as state feedback gives identical trajectories under every perturbation of state (CLAIM-522).

Construction 2: a transient encounter forms a maintained connector (A11, A12)

Encounter variables zᵢ decay (żᵢ = −zᵢ from 1), with intensity h = χ(z₁)χ(z₂), χ(z) = min{1, max{0, 10z − 5}}, which is zero after t = ln 2.

q̇ = (20h + 12q c₁c₂/(1 + c₁c₂))(1 − q) − q, ċ₁ = 4q c₂²/(1 + c₂²) − (1 + d₁)c₁, ċ₂ = 4q c₁²/(1 + c₁²) − (1 + d₂)c₂, from q = 0, c₁ = c₂ = 3.

  • Capture. The box [0.8, 1] × [1, 4]² is entered by t = ¼ (q(¼) ≈ 0.967) and is positively invariant for damage up to 0.4 after the encounter ends: inflow 0.2 at c = 1, 0.16 at q = 0.8. In the long run at d = 0.4, (q, c) ≈ (0.897, 2.085). Without the encounter, q = 0 is invariant and the capacities decay.
  • Knockouts. Removing any single production pathway sends all three to zero.
  • Fold. Symmetric positive equilibria: q = 11/12 − 1/(12c²), d(c) = (11c² − 1)/(3c(1 + c²)) − 1, maximal at c² = (7 + 2√15)/11: c ≈ 1.1578, q* ≈ 0.8545, d* ≈ 0.6908. The slowest maintenance eigenvalue goes to zero there.
  • Coupling at the fold. With L = q Bᵀ diag(c₁, c₂) B the spectrum at the fold is {0, qc, 3qc}, so λ₂ ≈ 0.9894 (CLAIM-521).

What it shows and does not

It shows a capacity to maintain, not only a state, being formed by a transient event, kept by what it enables, and lost past a threshold, with the coupling it supports unchanged up to that threshold. As A11 said, it “demonstrates emergence of an operative relation, not creation of a new fundamental law”. The capacities exist from the start in Construction 2; the encounter supplies only the connector, so this is a bistable system pushed across a separatrix. Which terms are internal is stipulated, the substrates are assumed available, and the production terms are not yet paid for thermodynamically. A13 said that a positive production rate is not yet a realizable mechanism, and Rao and Esposito make it exact: in an open, reversible mass-action network, sustained currents need an emergent cycle with nonzero affinity (LIT-1889, THEORY-1266). A12’s “viability kernel” over every disturbance is Aubin’s invariance kernel, not the viability kernel THEORY-134 defines.

Note of 2026-10-31: Construction 1 as reversible chemistry

The reading of the reaction-network works rewrote Construction 1 as reversible mass-action chemistry, with fuel S and waste W chemostatted, all rate constants 1 and [S] = 3. The results:

  • At zero affinity there is a single equilibrium, c = (3, 3), with no current and no extinct state.

  • Bistability appears only above about 3.52 RT of driving, that is [W] < 0.0887. This threshold belongs to this one reversible network with these parameters. It is not a general threshold for chemical bistability or for organizational maintenance.

  • The case’s equilibria, (3 ∓ √5)/2, return only in the limit [W] → 0, the limit of infinite affinity.

  • The maintained state costs dissipation equal to current times affinity, J_ε A_ε: 29.77 at [W] = 0.01.

  • There is no extinct state at finite affinity. With [W] > 0 the reverse of decay is a positive basal production, so the lower stable equilibrium is a low-activity branch with positive capacity, not zero. It approaches extinction only in the singular limit [W] → 0.

So the case’s maintained branch, and the collapse to a low-activity branch, are features of strong driving, not of the production graph alone. “Extinction” in the case is the infinite-affinity idealization. And maintenance that is “endogenous” relative to the organization lasts only while the reservoirs do. A chemostat is itself a finite-lived structure of a larger closed network, open for a time of order its abundance ratio (THEORY-1250).

Note of 2026-10-31: the folds are statements about infinite size

Read with the stochastic-thermodynamics works, both constructions are deterministic, so they hold in the limit of infinite size. At finite size a maintained regime is metastable.

  • Lifetime. It lasts a time exponential in size, set by a barrier in a quasi-potential computed from the dynamics, not by a free energy (THEORY-1273, THEORY-1264).
  • Near the fold. The barrier closes as the 3/2 power of the distance to the fold, so the hazard of escape rises steeply as the fold nears. Whether an observed transition comes before the fold is not fixed by that alone. It depends on system size, noise scale, how long the system is observed and how fast the parameter is changed.
  • Dissipation. The production and decay terms here are irreversible, so they have no defined entropy production. To be paid for in stochastic-thermodynamic terms, every step needs a reverse step obeying local detailed balance (LIT-1892, THEORY-1265).

Vellela and Qian’s Schlögl model (LIT-1890) is the chemical, stochastic counterpart of this case, as CASE-111 is its deterministic predecessor.

Three claims are to be kept apart:

  1. a deterministic saddle-node exists in the limiting model;
  2. a finite stochastic system can escape its metastable regime before that saddle-node;
  3. where the transition is observed depends on the finite-time protocol.

The constructions establish the first. The stochastic readings establish the second. The third is a matter of the experiment’s design.

Note of 2026-11-01: how-possibly models, and what the knockouts show

  • How-possibly. In Bechtel and Abrahamsen’s terms (LIT-1936, THEORY-1290) both constructions are de novo dynamical models. Their variables are posited, not properties of parts found by experiment. So they show how a maintained organization could behave (contributions C1 and C2), not that any system is organized this way.
  • The knockouts. Removing a production pathway and finding that maintenance ends is their C3, a clamp in a model (THEORY-1289). It shows the pathway is a component of the mechanism responsible for maintenance. It does not show the pathway is the organization’s own, since “Which terms are internal is stipulated”.
  • Provenance. The outside controller of CLAIM-522 meets mutual manipulability’s manipulability conditions as the internal pathway does. So which one is a constituent of the organization is settled by the declared boundary (CLAIM-530).

No status, title or warrant changes.

Note of 2026-11-03: not a new organization

A31 of the exchange “Assess SDT Coverage” (2026-11-02) read this case as an organization that “develops a dependency structure it did not previously possess”, “a genuinely self-maintaining organization”. The case says otherwise: “The capacities exist from the start in Construction 2; the encounter supplies only the connector”. It is the starting point for the construction CLAIM-532 calls for, in which the encounter would produce a new distinction and channel. That construction is CASE-191, a variant of this case with the encounter replaced by the agent’s own frustration.