How a Black Hole's Shadow Betrays Hidden Corrections express

Original: "Photon Spheres and shadow of modified black-hole entropies"
· Fang Liu, Yu-Bo Ma, Yun-Zhi Du, Huai-Fan Li
arXiv:2605.01303 · 2026-05-02 · CC BY 4.0 · 2 min
The shadow of the supermassive black hole at the center of the Milky Way helps test whether the horizon area formula holds.

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A black hole is like a perfect vault: everything that falls in disappears without a trace. But in the 1970s, Jacob Bekenstein and Stephen Hawking discovered that the horizon carries an indelible "sticker" — entropy (a measure of hidden information about swallowed matter). It turned out to be proportional to the horizon's area, not its volume, as with ordinary bodies. This rule — the Bekenstein–Hawking law — became a cornerstone of black hole physics.

However, under extreme conditions where quantum effects become important, the simple area formula may break down. Corrections appear — logarithmic or power-law additions to entropy. The authors of the new study asked: can these corrections be detected from outside, without peering beneath the horizon? They showed that modified entropy drags the metric along — the mathematical description of spacetime curvature around the hole. And the metric, in turn, affects how light bends around the hole and what shadow we see.

A black hole's shadow is not the hole itself but a dark silhouette against a bright ring of photons trapped in a circular orbit. The ring's radius is almost three times the horizon's.

The researchers calculated the photon sphere radius and shadow size for the corrected metric and compared them with the actual image of our galaxy's center — Sagittarius A* — obtained by the Event Horizon Telescope. It turned out that even small additions to entropy shift the shadow by an amount comparable to measurement precision. This allowed placing constraints on correction parameters: too strong deviations from the area law are simply incompatible with what we see.

Thus, the shadow of a black hole, frozen in a photograph, becomes a window into the world of quantum gravity. Like a barely visible scratch on a vault hints that the lock is more complex than it seemed.

The entropy of a black hole with the mass of the Sun is about $10^{77}$ times greater than that of the Sun itself. If our star collapsed into a hole, its "information capacity" would grow enormously — as if a planet-sized library turned into a point.

In Greg Bear's novel "The Light of Distant Stars," civilizations use black hole shadows as giant gravitational lenses for intergalactic communication, but they do not realize that the shadow's shape reveals fundamental corrections to the laws of thermodynamics.

S_{\text{BH}} = \frac{k_B c^3 A}{4 G \hbar}
Black hole entropy by Bekenstein–Hawking: S is entropy, k_B is Boltzmann's constant, c is the speed of light, A is the horizon area, G is the gravitational constant, ħ is the reduced Planck constant.
Scientists
Jacob BekensteinStephen HawkingFritz ZwickyKarl SchwarzschildSubrahmanyan ChandrasekharRainer Weiss
Concepts
photon sphere logarithmic correction black hole shadow anomalies Bekenstein-Hawking entropy black hole light bending entropic shadow hawking area law wald entropy horizon area schwarzschild radius schwarzschild metric kerr metric spin parameter quantum corrections photon photometry apparent horizon precision photometry modified gravity singularities hawking radiation anomalies