A(r)
D²(r), the positive lapse-like metric function in the diagonal ansatz. A→1/4 at the formal centre.
Search the vocabulary of SSZ, geometry, observables, testing and scientific status.
D²(r), the positive lapse-like metric function in the diagonal ansatz. A→1/4 at the formal centre.
Dimensionless segment-density field. Its operative form depends on the declared radial regime.
Dimensionless time factor 1/(1+Ξ), relating dτ to dt for static observers.
Golden ratio (1+√5)/2≈1.6180339887 used in the canonical strong branch.
Schwarzschild length scale 2GM/c².
Ricci scalar and Kretschmann scalar. In the current diagonal centre limit they diverge as r⁻² and r⁻⁴.
In PPN, γ and β are weak-field parameters and the declared completion uses γPPN=βPPN=1. In the pure metric’s flow module, \(\gamma_{\rm flow}=1+\Xi=D^{-1}\) and \(\beta_{\rm flow}=\sqrt{1-\gamma_{\rm flow}^{-2}}\). These meanings must never be mixed.
Redshift convention defined by \(1+z=\nu_e/\nu_o\). The identity z=1/D−1=Ξ applies only to a static emitter compared with a static observer at infinity.
Temporal and radial coefficients \(A=D^2\) and \(B=D^{-2}\). Their product is one in the current diagonal ansatz.
For the diagonal spherical form, \(\det g=-c^2D^2s^2r^4\sin^2\theta=-c^2r^4\sin^2\theta\). This exact cancellation tests algebraic coupling; it does not prove a regular centre.
The non-diagonal repository form with \(g_{tr}=\beta c\). The cross term belongs to a chosen coordinate representation and is not, by itself, rotation, frame dragging or material flow.
The tensor \(g^{\mu\nu}\) satisfying \(g_{\mu\alpha}g^{\alpha\nu}=\delta_\mu^{\ \nu}\). Passing this identity validates construction and inversion—not observational truth.
Normalised areal radius \(x=r/r_s\). Branch derivatives must state whether they are taken with respect to x or physical radius r.
The radius defined by a symmetry sphere’s area 4πr². Its zero is geometrically significant.
The currently selected source or definition within the project hierarchy. A later P0 correction can supersede an older file labelled canonical.
A chart failure removable by changing coordinates, unlike an invariant curvature divergence.
The quintic Hermite transition that matches Ξ, its first derivative and its second derivative at x=1.8 and x=2.2. Smooth joining does not derive a physical phase transition.
A dated execution with environment, command and outcome. The 1,296-pass record is a historical twelve-repository subset. The 9,300 figure is a catalogue of test/result artefacts, not a single executed run; 1,175 executed outcomes belong to a separate intermediate audit snapshot.
One assertion outcome under a named runner and environment. It is not interchangeable with a script, parameterisation, phase, log, report file or independent physical experiment.
A comparison whose data, uncertainties, nuisance parameters, flexibility and selection protocol are specified. Lower residuals in one pipeline remain conditional evidence until independently reproduced.
Data do not reject a model within a defined analysis. It is weaker than unique confirmation.
A global causal boundary, definable only from the full spacetime—not merely a zero or finite value of one local coefficient.
The stress tensor obtained by inserting the metric into a GR-style Einstein tensor. It diagnoses the geometry but is not a derived fundamental SSZ matter theory.
The complementary fall scale vfall = c√(r/rs) = c2/vesc. Its product with vesc is exactly c2. It is not a locally measured material 3-velocity and is distinct from the metric proxy c√(1−D2).
The existence of observations or mathematical results that could rule out a model.
Whether all inextendible geodesics have complete affine/proper parameter ranges. Finite coefficients do not prove it.
A tetrad in which an observer reports physical components. It separates local measurements from chart-dependent quantities such as dr/dt.
Historical material retained for development history but not used as current scientific authority.
A frozen formula/parameter/method specification used to make downstream results reproducible.
The physical type of measurement—static clock, null path, timelike orbit, wave or dataset fit—which determines the required forward model.
A test of how often one method wins within matched pairs. It does not measure effect size or correct automatically for selection, flexibility or correlation.
A highest-priority scientific clarification. Here it separates the repeatedly tested finite horizon factor from the unresolved construction of a physical global interior.
Parameterized post-Newtonian formalism for systematic weak-field comparisons.
The invariant time measured by a clock along a timelike worldline.
An areal centre with appropriate local geometry and finite curvature invariants—not merely finite metric components.
A declared formula-domain join, observable approximation boundary or physical transition. These three meanings are distinct and must be labelled.
A defined difference between data and model output. A small residual supports only that pipeline until uncertainty, covariance and alternative models are included.
Evidence that code satisfies specified tests. It is not direct evidence that nature selects the model.
A regime where weak-field expansions are insufficient and full metric/geodesic dynamics matter.
No. It is a concrete effective research programme with geometry, calculations and tests, but lacks a completed fundamental action, global interior and several dynamical sectors.
Tests repeatedly verify that the declared horizon time factor remains finite. The present diagonal extrapolation has divergent curvature at the areal centre, so that expression alone is not the completed interior. A different SSZ inner solution, matching construction or boundary geometry may still resolve the centre question; deriving and testing such a completion remains open research.
No local observer measures a vacuum light speed other than c. Coordinate speeds can change with coordinates and metric coefficients.
φ is structurally selected in the current branch. A deeper dynamical derivation of why nature should select it remains an open foundational question.
Locked strong-field forward predictions that fail sufficiently precise data, weak-field regressions, or a mathematical inconsistency in any proposed dynamical completion.
Different reports count functions, parameterised cases, custom phases, repositories or historical result artefacts. A valid total must state its scope and command.
The 9,300 figure is the catalogue of test/result artefacts, not a single executed run. A historical twelve-repository subset separately records 1,296 passed and zero failed. The full execution contains 5,294 unique repository/test definitions and 9,216 repository/file/test identities across 28 test-bearing repositories; execution is not the same as independent physical evidence. Repository-specific reruns remain separately visible, including 184/184 qubit and 54/54 Lagrange tests.
The finite horizon values and C² transition tests remain valid within their domains. The centre asymptotics evaluate a different locus and the present diagonal extrapolation. Future supplementary work can construct and test whether another SSZ interior completes the geometry.
No. Model flexibility, data selection, nuisance parameters, covariance and alternative models must be assessed independently.
This page separates the declared definition, its computation or visualisation, the evidence supporting it, and the conclusions that remain outside its scope.
Start with the formula or control, identify its domain and inputs, then follow the linked implementation and evidence record.
A passing identity, numerical limit, plot or comparison supports only the stated relation under its recorded assumptions and provenance.
It is not automatically an independent experiment, a complete physical theory, or a proof beyond the explicit claim boundary.
The portal keeps current canonical locks above historical descriptions and keeps software verification separate from empirical confirmation.
Use the current P0, JIF or mathematical lock for the formula and domain shown on this page.
Read tests, convergence, reference compatibility, dataset-conditioned comparisons and independent replication as different evidence classes.
Every result retains its assumptions, limits and explicit non-claim so a visual or passing assertion is not over-promoted.