Status: CANONICAL Paper: 21 — Interpretation of Gravitational Redshift
The gravitational redshift between two observers:
1 + z = D(r_obs) / D(r_emit) = (1 + Ξ_emit) / (1 + Ξ_obs)
For an observer at infinity (Ξ_obs → 0):
z(r) = 1/D(r) - 1 = Ξ(r)
The redshift equals the segment density! This is a clean, direct correspondence.
z_GR(r) = 1/√(1-r_s/r) - 1
z_SSZ(r) = Ξ(r)
z_GR ≈ r_s/(2r)
z_SSZ = Ξ_weak = r_s/(2r)
z_GR(r_s) = ∞
z_SSZ(r_s) = 0.802 (finite!)
| Object | M/M☉ | R (km) | r/r_s | z_GR | z_SSZ | Excess |
|---|---|---|---|---|---|---|
| PSR J0030+0451 | 1.44 | 13.02 | 3.06 | 0.219 | 0.328 | +50% |
| PSR J0740+6620 | 2.08 | 13.70 | 2.23 | 0.346 | 0.413 | +19% |
| PSR J0348+0432 | 2.01 | 12.50 | 2.10 | 0.380 | 0.457 | +20% |
| Hypothetical NS | 2.5 | 11.0 | 1.49 | 0.580 | 0.652 | +12% |
Systematic prediction: NS redshift +13% higher than GR. Testable with NICER.
SSZ predicts a discrete frequency scaling:
R = 1 + z = φ^N, N ∈ ℤ
This φ-grid is not a quantization of redshift but a preferred scaling at which segmentation effects align constructively.
Paper 10 introduces a curvature detection method using three-frequency comparison:
δ_AB = ln(ν_A / ν_B)
I_ABC = δ_AB + δ_BC + δ_CA
I_ABC = 0 → Flat spacetime
I_ABC ≠ 0 → Curved spacetime (segmented)
This provides a model-independent test for spacetime segmentation.
| Test | Repository |
|---|---|
| test_redshift.py | ssz-qubits |
| test_validation.py (GPS, PR, S2) | ssz-qubits |
© 2025–2026 Carmen N. Wrede, Lino P. Casu