Regime
boundaries
The strong and weak expressions are not switched at their raw intersection. A declared \(C^2\) bridge transports value, slope and curvature across \(1.8\le r/r_s\le2.2\). This page separates mathematical joins, physical interpretation and observable validity.
Values and derivatives through both joins
Move the probe to inspect the operative branch, \(\Xi\), \(D\), first derivative and numerical second derivative. The chart uses exactly the same field implementation as the main explorer.
Four questions that must remain separate
1 · Formula domain
Which declared branch is evaluated? This is fixed by \(x=1.8\) and \(x=2.2\) in the current piecewise implementation.
2 · Smoothness
Do value, slope and curvature match? The quintic bridge enforces six endpoint identities and removes artificial derivative jumps through second order.
3 · Observable regime
Is a weak-field expansion, static clock map, full geodesic integral or perturbation model required? The radial branch alone does not answer this.
4 · Physical transition
Does a genuine material, causal or dynamical phase boundary exist? The present bridge is an operational geometric prescription; a fundamental dynamics deriving it remains open.
What the C² constraint matches
| Location | Left description | Right description | Required continuity | What it does not prove |
|---|---|---|---|---|
| 1.8 rs | strong exponential branch | quintic bridge | Ξ, Ξ′ and Ξ″ | a dynamically generated phase change |
| 2.2 rs | quintic bridge | weak inverse-radius branch | Ξ, Ξ′ and Ξ″ | validity of weak-field observable shortcuts immediately at the join |
| rs | strong branch checkpoint | Ξ≈0.801711847; D≈0.555027709 | central regularity or a material horizon surface | |
| r→∞ | weak asymptotic limit | Ξ→0; D→1 | global completeness of the interior | |
Which machinery is valid where?
| Observable | Near/strong field | Transition | Far/weak field | Guardrail |
|---|---|---|---|---|
| Static clock comparison | full \(D(r)\) | full bridged \(D(r)\) | full D or controlled expansion | state both radii and kinematics |
| Radial null travel | integrate full metric | integrate full metric | full metric or justified PPN limit | coordinate slope is not local light speed |
| Lensing/Shapiro | full null geodesic model required | full null geodesic model required | PPN with declared geometry | never substitute a clock-only Ξ shortcut |
| Orbits | full effective potential and stability | full effective potential and stability | PPN or full geodesics | a named radius must carry metric variant and commit |
| Waves/QNM | perturbation equations needed | matching and dynamics needed | controlled approximation | proxy frequency is not a waveform |
How to read Regimes
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.
Definitions, evidence and limitations stay linked
The portal keeps current canonical locks above historical descriptions and keeps software verification separate from empirical confirmation.
Canonical source
Use the current P0, JIF or mathematical lock for the formula and domain shown on this page.
Evidence class
Read tests, convergence, reference compatibility, dataset-conditioned comparisons and independent replication as different evidence classes.
Boundary
Every result retains its assumptions, limits and explicit non-claim so a visual or passing assertion is not over-promoted.