The Black Hole Trampoline: A Jump Through the Horizon express

Original: "A smooth BTZ black bounce with an extremal null throat"
· Farzad Milani
arXiv:2608.04461v1 · 2026-08-05 · CC BY 4.0 · 2 min
Smoothing the horizon of a nonrotating BTZ black hole does not change the spacetime signature but creates a traversable wormhole.

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The idea was elegant: take a BTZ black hole (the three-dimensional analog of a regular black hole) and smooth its horizon with a special function. The hope was that inside, the spacetime signature might change — time becoming space, and space becoming time. But the calculations showed otherwise.

Instead of a signature change, the geometry turned into a 'black trampoline' (black hole with a traversable throat). If you switch to the coordinates of an infalling observer, spacetime continues beyond the horizon: there lies a second region, an exact copy of the exterior. The minimal throat radius (the narrowest point) sits at the horizon, and the singularity disappears. This is not curvature leading nowhere, but a bridge between two worlds.

The surface gravity at the horizon is zero — the black hole does not radiate, but the entropy of the throat is πrₕ/2G, which matches calculations by Wald and Cardy.

The authors computed the effective matter source that supports such a geometry and proved that all energy conditions are satisfied. Near the throat, spacetime becomes AdS₂ × S¹ — the product of two-dimensional anti-de Sitter space and a circle. Scalar perturbations are stable, but there is a peculiar Aretakis-type instability: the leading transverse derivative is conserved, while the next one grows linearly with time.

Attempting to smooth the gₜₜ component (as proposed for the Schwarzschild black hole) leads to a singularity at the horizon for any finite smoothing width.

The work did not confirm the signature-change hypothesis, but it provided an exact recipe for constructing a traversable wormhole from a BTZ black hole. This is important for understanding quantum gravity and the thermodynamics of horizons.

Original abstract

as written by the authors arXiv:2608.04461v1

We study a static, circularly symmetric deformation of the non-rotating BTZ black hole obtained by inserting a smooth transition function into the \emph{inverse} radial metric component, $$g^{rr}=S_\delta(r)F(r)$$ with $$S_\delta=\tanh[(r-r_h)/\delta]$$, leaving $$g_{tt}=-F$$ untouched. This was motivated by the proposal that such a construction realizes a Lorentzian-to-Riemannian signature change at the horizon; we show that it does not. In coordinates $$r-r_h=q^2$$ with an advanced time, the metric extends real-analytically across $$r=r_h$$, and the extension is Lorentzian: $$q=0$$ is a regular null hypersurface, a degenerate Killing horizon with vanishing surface gravity, beyond which lies a second, isometric copy of the exterior. The areal radius has a minimum there, so the geometry is a black bounce; the would-be Riemannian branch is a separate geometry the Lorentzian sector never reaches. We give the effective source in closed form, an invariant account of the energy conditions, and identify the near-throat geometry as AdS$$_2\times S^1$$. The scalar effective potential is proven strictly positive for every mode, and the throat circle is a minimal surface whose length gives an entropy $$\pi r_h/2G$$, reproduced independently by the Wald--Noether charge and by a Cardy estimate from the computed Brown--York mass -- concordant results for which no first law is available since $$\kappa=0$$. The throat carries an Aretakis-type instability, with a conserved leading transverse derivative and a linearly growing subleading one. We also record a negative result: smoothing $$g_{tt}$$ instead, as in the Lorentzian-Euclidean Schwarzschild proposal, is singular at the horizon for any finite smoothing width. We state explicitly what the construction does not establish.

The entropy of the throat of a BTZ black hole is proportional to the circumference of the throat, not the area, as in the four-dimensional case. In three dimensions, the horizon is a circle, not a sphere.

The idea of wormholes connecting different regions of space is familiar from the movie 'Interstellar', where heroes travel through a wormhole in search of a new home for humanity.

Scientists
Stephen HawkingJacob BekensteinFritz ZwickyKarl SchwarzschildSubrahmanyan ChandrasekharRainer Weiss
Concepts
schwarzschild black hole bardeen black hole schwarzschild metric horizon area event horizon stability innermost stable circular orbit Birkhoff's theorem gravitational singularity hawking area law black hole singularity airy disk constant flat space