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Cosmic sous-vide: How slow reheating resurrects primordial black holes

Original: "Reviving primordial black hole formation in slow first-order phase transitions"
· Wen-Yuan Ai, Ke-Pan Xie
arXiv:2605.11332v2 · 2026-05-11 · CC BY 4.0 · ⏱ 3 min · HEP Phenomenology Cosmology General Relativity
Gauge invariance and slow reheating during phase transitions in the early universe provide a new recipe for forming asteroid-mass primordial black holes, potentially accounting for all dark matter.
Abstract

In the early universe, first-order phase transitions (like water freezing, but on a cosmic scale) could have created clumps that collapsed into primordial black holes. Recent calculations showed that this mechanism fails when density contrast and collapse threshold are considered in a unified gauge (reference frame). A new study refutes that prohibition: after a supercooled state, slow reheating brings the universe into a matter-dominated epoch, where small perturbations have time to grow and collapse. Thus, primordial black holes once again become likely candidates for dark matter.

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In the seething cauldron of the early universe, the vacuum, like a supercooled liquid, could boil with bubbles of a new phase. For a long time, physicists pinned their hopes on these bubbles as a source of primordial black holes (PBHs)—ideal candidates for dark matter. Their invisible hand in spiral galaxies was first discerned by Vera Rubin. But recently the scenario almost got shelved: it turned out that the density contrast critical for collapse depends on gauge choice. In the physical comoving gauge, it turned out to be roughly an order of magnitude smaller than previously thought. It seemed that ghostly PBHs, once discussed by Stephen Hawking, would remain a hypothesis.

The breakthrough came when theorists realized that the key lay in the reheating rate. If a hidden sector interacts with our Standard Model only through weak kinetic mixing with a dark photon, then after the phase transition the universe does not flash instantly but smolders slowly. A matter-dominated era ensues, lasting more than a thousand Hubble times. This protracted pause is reminiscent of the artful sous-vide technique: no scorching flame—just a precise temperature at which even the toughest meat becomes tender. So it is with perturbations: in a rapid scenario they would burn up before having a chance to bloom, but here, like spices in a long slow simmer, they gradually gain strength and collapse into black holes. The mathematics of gravitational collapse, once developed by Kip Thorne in the context of gravitational waves, here finds new life.

Paradox: in the comoving gauge the density contrast is suppressed by a factor of 10, but the matter-dominated era stretches for thousands of Hubble times, and the faint whisper of inhomogeneities grows into the roar of collapse.

Numerical simulations of stochastic bubble nucleation show that for vacuum transition temperatures around 10⁶ GeV and a parameter β/H_n ≈ 8–18, asteroid-mass PBHs (10²⁰–10²² g) are born. These crumbs, weighing as much as a mountain but smaller than an atomic nucleus, could make up all dark matter. The scenario opens a double window for observations: future gravitational wave detectors could catch the ripples of their birth, leaving an imprint on the history of cosmic expansion.

Thus gauge invariance and slow reheating—yesterday's obstacles—become an elegant recipe for the birth of dark matter. The model entwines particle physics and cosmology, leaving intriguing questions: how do non-spherical collapse and angular momentum affect the outcome? What will the gravitational wave spectrum look like? In this slow cooking there are still many layers, but the main dish has already emerged: primordial black holes return to the scientific table. And while we wonder whether the darkness between stars is woven from these invisible crumbs, one detail is sobering: their birth requires energies millions of times higher than the reach of the Large Hadron Collider. The cosmic sous-vide operates at temperatures we cannot yet master.

🎯 A primordial black hole of asteroid mass (~10²⁰ g) would be the size of an atomic nucleus but weigh as much as a mountain. Passing through Earth, it would leave only a microscopic tunnel and a barely noticeable thermal trace—a true ghost, almost impossible to catch.

M_{\text{min}} \sim 10^{20}\,\text{g} \left(\frac{10^6\,\text{GeV}}{T_V}\right)^2
M_min is proportional to the square of the inverse vacuum transition temperature TV.
Scientists
Alan GuthAndrei LindeGeorges LemaîtreJames PeeblesAdam RiessBrian Schmidt
Tags
black hole gravitational waves dark matter big bang dark photon numerical simulation expansion of the universe Standard Model
Laws
Friedmann equationsHubble's lawHawking radiationgravitational lensingNoether's theoremBekenstein-Hawking entropy
Original: arXiv:2605.11332v2 · CC BY 4.0 · bridge42worlds