Now let’s ask the final natural question: If black holes really have finite absorbing cores instead of singularities, what predictions follow? Could we ever test this?
Core radius scaling The core radius depends on mass as
\[ r_c^3 = \frac{3 M c^2}{4 \pi \rho_c}. \]
Finite curvature at the core
Absorbing boundary condition
Infalling matter and radiation disappear into the core, not a singularity.
The boundary grows/shrinks according to
\[ \frac{dr_c}{dv} = \frac{\dot M c^2}{4\pi \rho_c r_c^2}. \]
Cosmology link
Tiny ratio of scales For a stellar-mass black hole:
\[ \frac{r_c}{r_h} \sim 10^{-23}. \]
Indistinguishable exterior
Cosmology
Quantum gravity phenomenology
Gravitational wave echoes?
The model does not make black holes observable in a new way today, the core is too small.
Instead, it gives a conceptually clean resolution of singularities:
It turns black holes from “mysteries hiding singular edges” into well-posed physical objects.
Symbol / Term | Meaning | Value | Metaphor |
---|---|---|---|
\(r_h\) | Horizon radius | \(2GM/c^2\) | Outer cloak of the black hole |
\(r_c\) | Core radius | \((3Mc^2 / 4\pi \rho_c)^{1/3}\) | Inner guardrail that prevents singularity |
\(\rho_c\) | Core energy density | Inflationary scale | Shared DNA with the early universe |
Echoes | Hypothetical GW reflections from near-horizon structure | Not expected here | Like sound bouncing in a canyon (but absent in our case) |
Cosmology link | Using \(\rho_c\) from inflation | Anchors predictions | A bridge between the smallest and largest scales |
The model resolves singularities while keeping exterior GR intact, with predictions tied to cosmology rather than astrophysical observations.