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How a Quantum “Pillow” Saves a Black Hole from Infinity ⚡ экспресс

Original: "Observational Constraints on Kazakov-Solodukhin Quantum-Deformed Black Holes from M87$$^*$$ and Sgr A$$^*$$ Shadows"
arXiv:2607.02631 · 2026-07-02 · CC BY · ⏱ 1 min · General Relativity
A quantum “pillow” turns the deadly infinity at a black hole’s center into a smooth bottom — and it shows in its shadow.
Abstract

Imagine a black hole where the central point of infinite density turns into a smooth ball of finite size—like a grain of sand softening a sharp edge. Scientists have studied such a quantum model: the singularity vanishes, the hole evaporates more slowly, and its shadow changes size. Will these quantum black holes become observable?

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At the center of a black hole, classical theory paints a point where density and spacetime curvature shoot to infinity — like an infinitely sharp needle. But quantum corrections, tracing back to the work of Karl Schwarzschild, add a tiny “pillow”: space cannot collapse to zero.

The needle turns into a smooth bowl — infinity vanishes.

Because of this, the “horizon” — the boundary of no return — shifts. The famous radiation discovered by Stephen Hawking weakens, and thermal characteristics become more stable. Even the black hole’s shadow — that dark silhouette — changes size, though it keeps its round shape. The biggest surprise: if the quantum pillow were just a bit thicker, the horizon could vanish entirely, exposing a calm core to the outside world.

🎯 If quantum corrections were slightly stronger, a black hole could lose its horizon entirely, exposing its smooth core to the outside world.

🎬 In the movie Interstellar, the heroes hope to unravel the quantum mysteries inside a black hole — and the new model makes that idea a bit less fantastic.

Scientists
Stephen HawkingJacob BekensteinAlbert EinsteinFritz ZwickyVera RubinBernhard Riemann
Tags
black hole spacetime curvature entropy
Laws
second law of thermodynamicsHawking radiationgravitational lensingBekenstein-Hawking entropyEinstein field equationsBoltzmann distribution
Original: arXiv:2607.02631 · CC BY · bridge42worlds