Skip to content
This repository was archived by the owner on Jul 7, 2026. It is now read-only.

Latest commit

 

History

History
109 lines (73 loc) · 3.46 KB

File metadata and controls

109 lines (73 loc) · 3.46 KB

Relation to General Relativity

Status: CANONICAL


SSZ as GR Extension, Not Replacement

A useful way to read SSZ is:

  1. GR provides a geometric description (curvature) that works extremely well
  2. SSZ keeps the successful GR structure in weak fields — identically
  3. 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.


Weak-Field Identity

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.


Strong-Field Differences

SSZ deviates from GR only in the strong field (r/r_s < ~10):

At the Schwarzschild Radius (r = r_s)

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

For Neutron Stars (r/r_s ≈ 2–3)

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.


D-Intersection Comparisons

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.


PPN Parameters

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.


Philosophical Difference

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

In One Sentence

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