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Smoldering Ember in a Star’s Heart: Two Apocalypse Scenarios

Original: "The Life and Death of Stars That Capture Primordial Black Holes"
arXiv:2606.02700v1 · 2026-06-01 · CC BY 4.0 · ⏱ 3 min · High Energy Cosmology Stellar General Relativity
Primordial black holes captured by stars can either quietly consume them over billions of years or set off a colossal explosion with powerful jets and gravitational waves.
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In the silent theater of the cosmos, a star’s life plays out over billions of years. But sometimes an invisible director sneaks onto the stage—a primordial black hole. This clump of dark matter, born in the first second of existence (as predicted by Stephen Hawking), with the mass of an asteroid and the size of an atom, can be captured by a star. Once inside, it slowly, like a smoldering ember beneath a velvet curtain, begins its journey to the core. Two finales await this stellar drama: a quiet fading or a deafening fireworks display that blows the roof off the theater.

Capture is a matter of chance and gravitational dance. Without a third partner—a giant planet (exoplanet)—the odds are negligible. Only the tidal forces of a gas world, like Jupiter, can slow down the wandering hole and lure it into the star’s gravitational trap. Then begins a slow migration to the center through dynamical friction—an effect mathematically described by Subrahmanyan Chandrasekhar. Over a timescale comparable to the Hubble time (discovered by Edwin Hubble), the hole reaches the core. In the core, the black hole triggers Bondi accretion: matter falls in almost spherically, but efficiency is low—the ember barely glows. If the hole doesn't gain enough angular momentum during the star's lifetime, the show ends without applause: the star quietly fades, and the hole remains in its remnants.

The scenario changes dramatically when the black hole’s mass exceeds 0.01–1 solar masses. Instantly, an accretion disk swirls around it—as if the curtain bursts into flames, opening the second act.

With the disk comes a magnetic field awakening, and jets ignite—relativistic plasma beams blasting along the spin axis. Their power, described by the Blandford–Znajek mechanism, reaches 10⁵⁰ erg/s—for a brief moment, brighter than an entire galaxy. In minutes, such a jet ejects more energy than the Sun will emit over its entire 10-billion-year life. The hole’s spin skyrockets to 0.8, and stellar matter scatters like a curtain ripped away by a hurricane. The flare is registered as a low-luminosity gamma-ray burst, with an ultraviolet peak and radio afterglow. No radioactive tail, typical of an ordinary supernova—just the clean signature of gravitational waves picked up by observatories like LIGO. Such a star death, ignited from within by dark matter, could explain some puzzling transients in astronomical archives.

This hypothesis weaves together three great mysteries: the nature of dark matter, the mechanisms of stellar explosions, and the origin of intermediate-mass black holes. If swarms of primordial black holes with asteroid masses indeed roam the Universe, then every red dwarf star or even our own Sun potentially carries such a parasite within. We may suspect nothing until next-generation gravitational-wave observatories hear the death chord of a star-devoured companion, and wide-field telescopes spot a flare where a harmless point of light shone just yesterday. The theater of the Universe is always full of invisible dramas—we just need to learn to watch and listen.

Monte Carlo simulations reveal that about half the time the explosive scenario triggers—the universe flips a coin whenever a star swallows a black hole.

🎯 If a primordial black hole of 10¹⁶ g mass lurked in the Sun’s center, it would grow so slowly that the disk stage would only arrive after 10 billion years. We wouldn’t even notice—until the very finale.

🎬 The image of a star devoured from within echoes Arthur C. Clarke’s novel Rendezvous with Rama, where an alien ship uses a black hole as an engine. And in Star Trek (2009), red matter creates black holes inside planets, causing them to implode.

R_B = \frac{2GM_{BH}}{c_s^2}
The characteristic accretion radius, defining the region where the black hole’s gravity dominates over the gas's thermal motion.
P = \eta_a \eta_\phi \dot{M}_{BH} c^2
The energy output of a rotating, magnetized black hole, where efficiency depends on spin and magnetic parameters.
Scientists
Christian DopplerD. B. McLaughlinDidier QuelozMichel MayorR. A. RossiterStephen Hawking
Tags
dark matter black hole gravitational waves supernova exoplanet LIGO asteroid red dwarf Sun
Laws
Doppler effectHawking radiationgravitational lensingBekenstein-Hawking entropyKepler's third lawEinstein field equations
Original: arXiv:2606.02700v1 · CC BY 4.0 · bridge42worlds