Tiny black holes explain galaxy flows and the expansion of the Universe express

Original: "More power on large scales"
· Jeremy Mould
arXiv:2601.07106 · 2026-01-12 · CC BY 4.0 · 1 min
Tiny black holes born at the Universe's dawn could explain why galaxies move faster and smooth out disagreements in expansion measurements.

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Dark matter may not be particles but black holes from the Big Bang era. In the early Universe, which was like a swirling batter, they were like heavy lumps — barely moving, they gathered surrounding matter and spun it into the swift galaxy flows astronomers observe today. But there's a twist: the lightest holes, according to Hawking's theory, evaporate, emitting energy. This evaporation gently warms the cosmic 'batter' in its early stages, thereby changing the calculated rate of the Universe's expansion and smoothing out the notorious tension between different measurement methods.

Astonishingly: a hole with the mass of an asteroid compressed to a point smaller than an atomic nucleus. Its slow evaporation could produce a mysterious glow in space.
Simulations showed: accounting for such holes removes the need to tweak other cosmological parameters, an elegant strike on two mysteries at once.

Original abstract

as written by the authors arXiv:2601.07106

The high value of the cosmic microwave dipole may be telling us that dark matter is macroscopic rather than a fundamental particle. The possible presence of a significant dark matter component in the form of primordial black holes suggests that dark halo formation simulations should be commenced well before redshift z = 100. Unlike standard CDM candidates, PBHs behave as dense, non-relativistic matter from their inception in the radiation-dominated era. This allows them to seed gravitational potential wells and begin clustering earlier. We find that starting N-body simulations at redshifts even before matter-radiation equality yield galaxy bulk flow velocities that are systematically larger than those predicted by standard LCDM models. The early, high-mass concentrations established by PBHs lead to a more rapid and efficient gravitational acceleration of surrounding baryonic and dark matter, generating larger peculiar velocities that remain coherent over scales of hundreds of Mpc. Furthermore, a sub-population of PBHs in the 10^-20 to 10^-17 solar mass range would lose a non-negligible fraction of their mass via Hawking radiation over cosmological timescales. This evaporation process converts matter into radiation, so a time-varying matter density parameter, Omega_m', is introduced, which behaves like a boosted radiation term in the Friedmann equation. This dynamic term acts to reduce the Hubble tension. A higher effective Omega_r in the early universe reduces the sound horizon at the epoch of recombination. PBH mass loss also influences fits to the equation of state parameter, w, at low redshift. The naive N-body modelling presented here suggests investigation with tried and tested cosmology codes should be carried out, by introducing mass losing PBHs and starting the evolution as early as practicable.

One such hole weighs as much as an asteroid but is compressed to a point smaller than an atomic nucleus. Its evaporation is so unhurried that over the entire history of the Universe, it would lose only a minuscule fraction of its mass.

Scientists
Stephen HawkingJacob BekensteinVera RubinFritz ZwickyKarl SchwarzschildSubrahmanyan Chandrasekhar
Concepts
dark matter subhalo early dark energy early universe black holes black hole memory burden radiation dominated era ecdm model lcdm model neutron star mass limit mass ratio cosmological parameters matter density critical collapse primordial gravitational waves primordial magnetic fields no-hair theorem density profile negative energy metal poor reheating cosmic microwave background measurement