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Quantum Cloud Near a Black Hole ⚡ экспресс

Original: "Fermion condensate at the event horizon"
arXiv:2605.21064 · 2026-05-20 · CC BY 4.0 · ⏱ 1 min · General Relativity
Modified rules for lone particles predict a cloud at the very edge of a black hole.
Abstract

The standard anticommutation relations for fermions (rules governing particles with half-integer spin) can be modified in curved spacetime near a black hole's horizon. It is shown that such a modification leads to stationary solutions for the two-point Green's function, which describes particle propagation. These solutions are interpreted as a fermion condensate — a stable "cloud" of particles right at the horizon. This condensate may play a role in black hole evaporation processes.

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In the micro-world, solitary particles — fermions — avoid each other. This principle is at the heart of modern physics and makes electrons keep their distance, giving atoms their bulk. But near a black hole, spacetime is so warped that the usual laws collapse.

Physicists modified the equations and found that on a tight 'bend' at the event horizon — the point of no return — fermions get stuck, forming a gridlock. This particle cloud, a motionless condensate, is like a quantum atmosphere of the black hole.

This traffic jam isn't just a mind game. It could slightly blur the famous shadow of the black hole snapped by the Event Horizon Telescope. Schwarzschild and Hawking laid the foundations, while Wheeler coined the term for these objects. Now we're adding a detail that weaves into the images.

🎯 Fermion particles, like electrons, can't stand neighbors: two identical ones will never be in the same spot. This gives atoms their volume. At a black hole's horizon, this rule breaks down.

🎬 This cloud echoes the sci-fi idea of 'quantum foam' — a shifty reality on the brink of the abyss.

Scientists
Stephen HawkingJacob BekensteinAlbert EinsteinFritz ZwickyVera RubinEmmy Noether
Tags
black hole spacetime curvature Standard Model
Laws
Hawking radiationgravitational lensingNoether's theoremBekenstein-Hawking entropyEinstein field equationsequivalence principle
Original: arXiv:2605.21064 · CC BY 4.0 · bridge42worlds