Shadow and Ring: How to Weigh a Black Hole More Precisely ✎ express

Original: "Prospects for Improving the Theoretical Uncertainty for Tests of General Relativity with the EHT"
arXiv:2606.30753 · 2026-06-29 · arXiv non-exclusive · independent analysis · 2 min
Comparing the bright ring in a black hole image with its mathematical shadow helps us weigh the abyss more accurately.

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At the center of galaxy M87, 55 million light-years away, lurks a black hole with a mass of 6.5 billion Suns. In 2019, the Event Horizon Telescope (EHT) gave us its first portrait: an orange donut with a dark core. But the donut is not the abyss itself. It is glowing gas heated to billions of degrees, swirling before vanishing forever. The true shadow is slightly smaller than the ring, and its size is encoded in the radiation.

Astrophysicists built thousands of computer simulations of accretion disks — differently twisted, magnetized, and tilted relative to the observer. Each simulation produced its own ring and shadow. By comparing them, the authors derived a calibration curve: how to recover the true shadow size from the measured ring. They found that the uncertainty can be reduced severalfold by observing at 345 GHz (nearly twice the current frequency), using geometric constraints from the PRIMO algorithm, and accounting for the fact that the black hole's spin axis in M87 nearly aligns with the direction of the giant jet — a plasma stream thousands of light-years long.

The difference between the shadow and the ring is like the difference between a person's silhouette and their photo in a crowd. The silhouette is sharp, but in the photo we only see the outline of neighbors standing close.

The most unexpected helper in this work is 'time-delay filtering.' Instead of just measuring the ring's size, we track how stable that size remains from frame to frame. The ring's jitter reveals gas turbulence, while its stability reveals the black hole's own geometry. According to the authors' calculations, this approach can make the calibration even more precise with each new EHT observing run.

The magnetic field in the disk can be so strong that it prevents gas from falling in all at once: it accumulates and then breaks through, like water behind a dam. This regime is called a magnetically arrested accretion disk.

When the black hole's mass is known from other measurements, the refined ring–shadow relation becomes a test of general relativity. If the shadow turns out not to be where predicted, then gravity near the event horizon works differently than we thought. So far, all checks confirm Einstein, but precision is increasing, and each new image is a step toward spotting a deviation if it exists.

The black hole's shadow is about 2.6 times larger than the event horizon — due to the strong bending of light rays by gravity.

In the movie 'Interstellar,' the visualization of the black hole Gargantua is based on real calculations of light bending, and its bright ring closely resembles the EHT images.

Scientists
Jacob BekensteinStephen HawkingFritz ZwickyKarl SchwarzschildSubrahmanyan ChandrasekharRainer Weiss
Concepts
black hole shadow black hole entropy EHT logarithmic correction schwarzschild metric schwarzschild radius image quality gravitational radius mass ratio reverberation mapping charge to mass ratio barrow entropy apparent horizon cosmic expansion uncertainty effective spin event horizon stability entropic shadow kerr metric Hawking area theorem quantum gravity and symmetry