Status: CANONICAL
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
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
Ξ_weak(r) = r_s / (2r)
Recovers GR to arbitrary precision. PPN parameters β = γ = 1 (exact).
Ξ_strong(r) = 1 - exp(-φ · r_s / r)
Saturates at Ξ_max. Finite time dilation at all radii.
Hermite C² interpolation ensures continuous Ξ, dΞ/dr, d²Ξ/dr².
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.
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.
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 derivedD_SSZ = D_GRcomparisons 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.
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.
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.
| # | 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