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Core Postulates of SSZ

Status: CANONICAL


Postulate 1: Segment Density Field

There exists a dimensionless, non-negative scalar field Ξ(r) (segment density) that characterizes the degree of spacetime segmentation at radial coordinate r from a gravitating mass.

  • Ξ is determined by mass M and radius r (not freely tunable)
  • Ξ ≥ 0 everywhere
  • Ξ → 0 as r → ∞ (flat spacetime limit)
  • Ξ is bounded: Ξ ≤ Ξ_max = 1 - e^(-φ) ≈ 0.80171

Postulate 2: Modified Time Dilation

The SSZ time-dilation factor is:

D_SSZ(r) = 1 / (1 + Ξ(r))

This replaces the GR expression D_GR(r) = √(1 - r_s/r) in the strong field while converging to it in the weak field.

Consequences:

  • D(r→∞) = 1 (no dilation far from mass)
  • D(r_s) = 0.55503 (finite, not zero!)
  • D is monotonically increasing with r
  • No singularity at any finite r

Postulate 3: Two-Regime Structure

g1 — Weak Field (r/r_s > 2.2)

Ξ_weak(r) = r_s / (2r)

Recovers GR to arbitrary precision. PPN parameters β = γ = 1 (exact).

g2 — Strong Field (r_s/r < 1.8)

Ξ_strong(r) = 1 - exp(-φ · r_s / r)

Saturates at Ξ_max. Finite time dilation at all radii.

Transition (1.8 ≤ r/r_s ≤ 2.2)

Hermite C² interpolation ensures continuous Ξ, dΞ/dr, d²Ξ/dr².


Postulate 4: φ-Geometry Constraint

The golden ratio φ = (1+√5)/2 = 1.618... enters as a structural constant, not a free parameter:

  • Ξ_strong uses φ as exponential scale
  • Coupling radius: r_φ = (φ/2) · r_s · [1 + β · Δ(M)]
  • φ/2 = 0.80902 appears as coupling factor
  • The ratio φ constrains regime transitions and scaling behavior

This is treated as a constraint that reduces arbitrariness, not numerology.


Postulate 5: Observable → Method Assignment

Not all observables use the same formula. SSZ mandates:

Observable Type Method Formula
Timelike (clocks, redshift) Ξ-based D = 1/(1+Ξ)
Null (light: lensing, Shapiro) PPN (1+γ) result = Ξ_only × (1+γ)
Orbit (precession) PPN (β,γ) Standard PPN machinery

This is the Prime Directive: Never use a single method for all observables.


Postulate 6: No Free Parameters

SSZ has exactly zero tunable fitting parameters:

  • φ is a mathematical constant
  • β, γ are PPN parameters (both = 1)
  • Formula-domain boundaries are fixed by the canonical 1.8/2.2 blend rule; r* values are derived D_SSZ = D_GR comparisons for declared Xi forms
  • Mass-dependent correction Δ(M) follows from φ-geometry

If SSZ predictions are wrong, SSZ is wrong — there is no knob to turn.


Postulate 7: Irreversible Coherence-Collapse

The transition from g1 to g2 is unidirectional:

g₁ → g₂: Irreversible (not reversible)

Once spacetime segmentation reaches the strong-field regime, it does not spontaneously return to the weak-field state. This is a thermodynamic-style arrow, not a dynamical instability.


Postulate 8: Anti-Circularity

SSZ formulas must never be calibrated against the data they are used to predict. Every prediction follows from:

Mass M → r_s → Ξ(r) → D(r) → Observable

The chain is one-directional. Reverse inference (observable → Ξ → M) is used only for consistency checks, never for calibration.


Summary Table

# Postulate Expression
1 Segment density Ξ(r) ≥ 0, bounded
2 Time dilation D = 1/(1+Ξ)
3 Two regimes g1: weak, g2: strong
4 φ-constraint φ as structural constant
5 Method assignment Observable → Class → Method
6 No free parameters Zero tunable knobs
7 Irreversible g1→g2 Coherence-collapse law
8 Anti-circularity No data → formula feedback

© 2025–2026 Carmen N. Wrede, Lino P. Casu