Structural Postulates

Each derivation that requires assumptions beyond the three axioms makes them explicit as structural postulates. These specify the mathematical setting in which the derivation operates — they are not derived from the axioms, but they are motivated by the framework's structure. The majority of derivations require no additional assumptions at all.

15 postulates originally introduced as assumptions have since been derived as theorems from earlier results, reducing the framework's independent assumptions.

5
Active postulates
15
Now theorems
5
Derivations with active
56
Derivations without

Foundation

S1 Finite-dimensional manifold Now a theorem

The state space Σ is a finite-dimensional compact smooth manifold. Now derived as Theorem 0.2: the base case S¹ is a Lie group manifold (from U(1) loop closure), the inductive step uses level sets of relational invariants (regular value theorem preserves manifold structure), and finite dimensionality follows from the Delone finite local complexity of the observer network.

Promoted to Theorem 0.2. The manifold structure follows from the constructive mechanism by which observer state spaces are built: U(1) Lie group orbits at the base, bootstrap level-set construction at each step, finite local complexity from aperiodic order bounding the dimension.

S2 Invariant Riemannian metric Now a theorem

A Riemannian metric g on Σ that is G_O-invariant: φ_t* g = g for all t.

Now a theorem (Theorem 0.1): any smooth compact manifold admits a Riemannian metric (partition of unity), and Weyl averaging over the compact U(1) action produces a G_O-invariant metric. Replaces the former structural postulate.

Dynamics

S1 Symplectic structure Now a theorem

The joint state space Σ₁ × Σ₂ carries a symplectic form ω compatible with the U(1) × U(1) action of the constituent observers.

Now a theorem (Theorem 0.1): Axiom 3 gives each observer a Noether pair (Loop Closure, Theorem 3.1), a Noether pair defines a symplectic form, and the product of symplectic manifolds is canonically symplectic (Abraham & Marsden, Proposition 3.2.10).

S1 Smooth coherence measure Now a theorem

The coherence measure C is at least C² (twice continuously differentiable), with a positive-definite Hessian metric on state space.

Now a theorem (Theorem 0.1): the Born Rule (derived via coherence-operational) forces statistical regularity for finite-dimensional systems, and the Fisher metric chain (Čencov uniqueness + Proposition 4.1 of Fisher Information Metric) identifies the coherence Hessian as ℏ × Fisher metric, which is C∞ and positive definite.

Geometry

S1 Smooth ambient geometry

The ambient multi-observer coherence geometry is a smooth manifold. TIGHTENED: individual state space smoothness is derived (Loop Closure Theorem 0.2), quadratic form from U(1) isotropy, Lorentzian signature from causal structure. The irreducible content is: the global assembly of the observer network into a smooth ambient manifold. Reduces to the continuous-discrete duality compatibility condition (Conjecture 4.1).

Individual observer state spaces are smooth manifolds (Theorem 0.2). Geometric connections between them are smooth (ER=EPR). The remaining question is whether the global assembly produces a smooth manifold, which is the continuous-discrete duality’s compatibility condition.

S1 Homogeneity Now a theorem

The coherence measure C and the metric g are invariant under spacetime translations xμ → xμ + aμ.

Follows from the axioms' location-independence: coherence conservation and observer definitions do not reference absolute position, so the derived geometry inherits translation symmetry.

S1 Metric–density coupling Now a theorem

The metric g_μν is locally determined by the relational invariant density ρ_I, with curvature proportional to ρ_I.

Derived from coherence subadditivity (Axiom 1, C4): the action duality links the spacetime metric to the coherence Hessian; subadditivity ensures the Hessian varies with observer content; action equality transfers this to the spacetime metric. Locality from finite c; coupling to ρ_I from Noether identification.

S1 Second-order locality Now a theorem

The self-consistency relation between curvature and coherence content involves at most second derivatives of the metric g_μν.

Now a theorem (Coherence Lagrangian, Theorem 6.0): Ostrogradsky's instability theorem shows higher-derivative Lagrangians have unbounded Hamiltonians, violating the Lyapunov stability required by Axiom 3 (loop closure). Second-order locality is therefore forced by loop closure stability.

Quantum

S1 Amplitude–coherence identification Now a theorem

The coherence measure restricted to transition amplitudes satisfies C(|ψ⟩) = ⟨ψ|ψ⟩ = Σ_k |ψ_k|².

Now a theorem (Theorem 0.1): the unique continuous, U(1)-invariant, composition-compatible coherence functional on quantum states is the squared norm, via the Cauchy multiplicative equation. Derived in Coherence as Physical Primitive (Theorem 4.1).

S1 Interaction–invariant correspondence

Every Type III interaction generates a relational invariant whose operator representation is the conserved quantity associated with the interaction Hamiltonian via Noether's theorem. TIGHTENED: the structural correspondence (invariants map to conserved quantities) is forced by the continuous-discrete duality. The irreducible postulated content is the explicit map from interaction configurations to specific Hamiltonians.

The continuous-discrete duality forces relational invariants (discrete layer) to map to conserved quantities (continuous layer) — there is nothing else in the Lagrangian dynamics for them to correspond to. What remains postulated is the specific identification of which Hamiltonian governs which interaction.

Particles

S1 Topological consistency Now a theorem

Transition amplitudes are single-valued on the universal cover of configuration space. The wave function is a section of a flat line bundle with holonomy Hom(π₁(Q), U(1)).

Now a theorem (Theorem 0.1): Axiom 3 (loop closure) applied to configuration space forces single-valued phases on the universal cover; the holonomy classification follows from standard covering-space theory. The Laidlaw–DeWitt condition is derived, not postulated.

S1 Tunneling–crystallization correspondence

The formation of stable composite observers at each bootstrap level is mediated by coherence tunneling through a barrier in the coherence geometry. TIGHTENED: the WKB form of the tunneling probability is a theorem of semiclassical analysis for any Lagrangian system (the coherence Lagrangian provides the Lagrangian). The irreducible postulated content is the identification of bootstrap crystallization with barrier tunneling.

The exponential WKB suppression is forced by the Lagrangian dynamics (Coherence Lagrangian, Theorem 6.0). What remains postulated is that composite observer formation at each bootstrap level corresponds to barrier penetration in the coherence geometry.

S1 Generation–axis correspondence Now a theorem

Each fermion generation corresponds to a class of half-integer winding loops classified by dominant alignment with one of three independent generators of so(3), partitioned by Voronoi decomposition of S².

Since d = 3 spatial dimensions provide exactly three independent rotation axes, the half-integer winding loops of fermions naturally partition into three sectors, one per generation.

Gauge

S1 Locality of phase comparison Now a theorem

Phase comparison between observers at distinct spacetime points requires smooth parallel transport, described by a connection 1-form A on a principal U(1) bundle P → ℳ over the spacetime manifold.

Now a theorem (Theorem 0.1): local gauge freedom is inevitable from relational physics + finite signal speed (Theorem 2.1), and the classification theorem for connections on principal bundles (Kobayashi & Nomizu) shows the principal U(1) bundle with connection is the unique smooth implementation.

S2 Minimal gauge dynamics Now a theorem

The self-consistency condition for the U(1) gauge connection involves at most second derivatives of A_μ — equivalently, at most first derivatives of F_μν.

Now a theorem (Coherence Lagrangian, Theorem 6.0): Ostrogradsky instability excludes higher-derivative gauge Lagrangians, as the resulting unbounded Hamiltonian violates loop closure stability (Axiom 3).

S1 Algebraic completeness of phase structure Now a theorem

The observer’s phase algebra 𝒶 forms a normed division algebra over ℝ: for all a, b ∈ 𝒶, |ab| = |a| · |b|. Combined with three independent imaginary units (one per spatial axis), this selects 𝒶 = ℍ (quaternions).

Packages three physical requirements: (i) bilinearity of phase composition, (ii) norm-preservation from coherence conservation, (iii) invertibility of phase transformations. With exactly three imaginary units, Hurwitz’s theorem uniquely selects the quaternions.

S2 Minimal non-abelian gauge dynamics Now a theorem

The self-consistency condition for the SU(2) gauge connection involves at most second derivatives of Wᵃ_μ — equivalently, at most first derivatives of the field strength Wᵃ_μν.

Now a theorem (Coherence Lagrangian, Theorem 6.0): Ostrogradsky instability excludes higher-derivative gauge Lagrangians, as the resulting unbounded Hamiltonian violates loop closure stability (Axiom 3).

S1 Algebraic saturation at each bootstrap level Now a theorem

Each level of the bootstrap hierarchy saturates the phase algebra to the next normed division algebra via the Cayley-Dickson construction: ℝ → ℂ → ℍ → 𝕆. Hurwitz’s theorem terminates the sequence at 𝕆.

Extends the algebraic completeness postulate (Weak Interaction S1) to the full bootstrap hierarchy. Now derived as a theorem: Bootstrap → Division Algebras proves that coherence conservation forces Cayley-Dickson doubling at each level.

S1 Vacuum coherence minimization

In the confining phase, the vacuum state minimizes the total coherence cost subject to the constraint that all asymptotic states are color singlets.

Extends the bootstrap self-consistency principle to the non-perturbative regime: the vacuum should be the state of minimal coherence cost, generalizing the perturbative requirement to the confining phase.

Holography

S1 Planck-scale resolution

The coherence geometry has a minimum resolvable scale ℓ_P = √(ħG/c³). TIGHTENED: ℓ_P is dimensionally unique and is a fixed-point property of the self-consistency equation G = ℓ_min² c³/ħ. The irreducible postulated content is equivalent to the bootstrap fixed-point uniqueness conjectures (7.1–7.2). If those are proved, this becomes a theorem.

The Planck length is the unique length from ħ, G, c. The Jacobson route (Gravitational Coupling, Theorem 3.3) gives G = ℓ_min² c³/ħ, making ℓ_P a fixed-point property. The geometric substrate identifies ℓ_P with individual substrate nodes. The remaining content is the uniqueness of the bootstrap fixed point.