Status: CANONICAL
A useful way to read SSZ is:
- GR provides a geometric description (curvature) that works extremely well
- SSZ keeps the successful GR structure in weak fields — identically
- SSZ adds one extra operational layer — a segment density field Ξ — whose primary observational footprint is modified time dilation, saturating in strong fields
SSZ is not "anti-GR." It is closer to "GR + structured strong-field correction," with an explicit cap that avoids runaway divergences.
In the weak field (r/r_s > 2.2), SSZ and GR are identical to observational precision:
| Observable | GR | SSZ | Difference |
|---|---|---|---|
| GPS time correction | 45.85 μs/day | 45.85 μs/day | < 1 ns/day |
| Pound-Rebka Δν/ν | 2.46×10⁻¹⁵ | 2.46×10⁻¹⁵ | < 0.01% |
| Mercury perihelion | 42.98"/century | 42.98"/century | 0.00% |
| Eddington lensing | 1.75" | 1.75" | 0.00% |
| Cassini Shapiro γ | 1.000021 | 1.000021 | 0.00% |
| S2 star redshift | 0.00018 | 0.00018 | < 0.01% |
SSZ is designed to pass every existing weak-field test exactly.
SSZ deviates from GR only in the strong field (r/r_s < ~10):
| Property | GR | SSZ | Interpretation |
|---|---|---|---|
| Time dilation D | 0 | 0.555 | Finite vs infinite |
| Redshift z | ∞ | 0.802 | Bounded vs divergent |
| Proper time τ | 0 | > 0 | Observable vs frozen |
| Singularity | YES | NO | SSZ resolves it |
| Energy conditions | Violated | Satisfied | SSZ is regular |
| Object | z_GR | z_SSZ | Excess |
|---|---|---|---|
| PSR J0030+0451 (r/r_s=3.06) | 0.219 | 0.328 | +50% |
| PSR J0740+6620 (r/r_s=2.23) | 0.346 | 0.413 | +19% |
| PSR J0348+0432 (r/r_s=2.10) | 0.380 | 0.457 | +20% |
Systematic prediction: NS redshift +13% higher than GR — testable with NICER.
SSZ and GR agree at mass-independent comparison radii. The numerical value depends on the declared Xi form:
r*/r_s = 1.594811, D* = 0.610710 for Xi_A(x)=1-exp(-phi/x)
r*/r_s = 1.386562, D* = 0.528007 for Xi_B(x)=1-exp(-phi*x)
These intersection points are:
- Mass-independent (purely geometric)
- Derived from
D_SSZ = D_GR, not fitted - Meaningful only when the Xi form is stated
They are not hard regime boundaries. The operative blend remains fixed at 1.8 <= r/r_s <= 2.2.
| Parameter | GR | SSZ | Measurement |
|---|---|---|---|
| β | 1 | 1 (exact) | — |
| γ | 1 | 1 (exact) | Cassini: 1.000021 ± 0.000023 |
SSZ is PPN-identical to GR. All Solar System tests are passed by construction.
| Aspect | GR | SSZ |
|---|---|---|
| Core object | Metric tensor g_μν | g_μν + Ξ(r) |
| Singularities | Present at r_s | Absent (D > 0 everywhere) |
| Information paradox | Problematic | Avoided (finite D) |
| Falsifiability | Weak-field confirmed | Explicit strong-field predictions |
| Free parameters | 0 | 0 |
| Strong-field behavior | Divergent | Saturating |
SSZ = GR in the weak field + bounded segment density in the strong field, with zero free parameters and explicit falsification targets.
© 2025–2026 Carmen N. Wrede, Lino P. Casu