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Black Holes on the Brane: Images and the Search for Hidden Dimensions

Original: "Images of Braneworld black holes with radiatively inefficient accretion flows"
arXiv:2606.26166 · 2026-06-24 · CC BY · 3 min · General Relativity High Energy HEP Theory
Simulations of emission from accretion disks around brane black holes show that deviations from classical shadows are minimal, but future next-generation telescopes may discern them.
Abstract

Modeling black hole images on horizon scales opens the way to rigorous tests of gravity in the strong-field regime. The Casadio–Fabbri–Mazzacurati (CFM) black hole in the braneworld model contains an extra parameter characterizing tidal effects of the bulk geometry. General relativistic radiative transfer modeling was performed, and synthetic images were constructed, consistent with observations of M87* by the Event Horizon Telescope. It was found that the tidal parameter causes non-monotonic changes in shadow morphology, indicating a complex connection between the geometry of spacetime and the radiation from accreting plasma. Analysis of comparison metrics using normalized cross-correlation coefficients and DSSIM index showed that mismatch values reach on the order of 10^3, meaning that identifying braneworld black holes from their images remains a challenging task even with future ngEHT and BHEX observations.

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Context

General relativity of Einstein remains unsurpassed, but faces problems of singularities and dark matter. Brane scenarios, originating from string theory, offer an elegant extension: our Universe is merely a three-dimensional surface in a multidimensional bulk, and only gravity can penetrate extra dimensions. The search for observational traces of such models is one of the key tasks of modern astrophysics, especially in the era of direct images of black holes obtained with radio astronomy and interferometry.

Methods

The authors built a semi-analytical model of a radiatively inefficient accretion disk, where hot plasma radiates synchrotron emission at 230 GHz, matching the operating parameters of the Event Horizon Telescope. Using numerical simulations of radiation transport in curved spacetime, synthetic images were generated for CFM brane black holes, whose metric generalizes the Schwarzschild solution via the tidal parameter γ. The plasma motion was interpolated between Keplerian rotation and free fall, and the electron temperature reached a hundred billion Kelvin. Dependence on disk thickness and inclination angle to the observer was also accounted for.

Results

It turned out that varying the tidal parameter γ causes non-monotonic changes in the morphology of gravitational lensing rings: peak brightnesses and profile widths depend differently on the viewing angle and disk thickness. Relativistic asymmetry, caused by the Doppler effect and gravitational lensing, is enhanced on the approaching side of the disk. Comparison with M87* data using nCCC and DSSIM metrics showed that the quantitative image discrepancy does not exceed a few thousandths — about 0.1%. Even considering ambitious projects like ngEHT and BHEX, capable of reaching 5 microarcsecond resolution, identifying the brane nature remains extremely challenging. Curiously, at extreme values of γ (above 4) the black hole turns into a wormhole, but within the studied range the Hawking temperature, described by the Hawking radiation law and the work of Hawking, drops all the way to zero as the critical value is approached.

Implications

The results underscore that direct images of black holes cannot yet reliably distinguish the brane model from standard GR, posing an ambitious task for future instruments. Nevertheless, the discovered sensitivity of the shadow to the tidal parameter opens a fundamental possibility for testing multidimensional theories without resorting to colliders.

Future development

Further development will require accounting for radiation polarization, full-scale MHD simulations, and likely combining with gravitational wave observations. If future telescopes like BHEX can resolve higher-order photon rings, the chances of spotting deviations will increase by orders of magnitude.

Impact

The work stimulates the development of strong-field gravity testing methods and also influences the interpretation of Event Horizon Telescope data and the planning of next-generation missions.

Next steps

The researchers plan to incorporate polarization effects into the model and perform a Bayesian analysis on the entire EHT dataset to set upper limits on the tidal parameter.

Key open problems

Brane black holes are directly linked to attempts to unify quantum mechanics and gravity, as well as to the nature of hidden mass — in some scenarios, extra dimensions mimic dark matter. Successful detection of the tidal parameter would be the first evidence of the existence of other dimensions.

🎯 If the tidal parameter γ exceeds 4, the black hole turns into a traversable wormhole — an object capable of connecting distant regions of space, akin to those described in science fiction.

🎬 In the film Interstellar, a wormhole serves as a portal to planets in another galaxy; brane solutions allow such tunnels within the theory if tidal effects are large enough.

ds^2 = \left(1-\frac{2M}{r}\right)dt^2 - \frac{1-\frac{3M}{2r}}{\left(1-\frac{2M}{r}\right)\left(1-\frac{\gamma M}{2r}\right)}dr^2 - r^2 d\theta^2 - r^2\sin^2\theta d\phi^2
spacetime interval
T_{BH} = \frac{1}{8\pi M}\sqrt{1-\frac{3(\gamma-3)}{2}}
black hole temperature

Key numbers

  • mass of M87* black hole: 6.4×10^9 M☉
  • distance to M87*: 16.9 Mpc
  • image discrepancy magnitude: ~10⁻³
  • electron temperature in the disk: ~10¹¹ K
  • observation frequency: 230 GHz
Scientists
Stephen HawkingJacob BekensteinAlbert EinsteinFritz ZwickyVera RubinBernhard Riemann
Tags
black hole Accretion disk plasma gravitational lensing numerical simulation string theory Wormhole radio astronomy interferometry
Laws
Hawking radiationgravitational lensingBekenstein-Hawking entropyEinstein field equationsvirial theoremno-hair theorem
Original: arXiv:2606.26166 · CC BY · bridge42worlds