Rogue Black Holes: Dark Matter Doesn't Fuel Their Growth ✛ ✎ ✦

Original: "Variability in Supermassive Black-Hole Accretion Rates in Fuzzy Dark Matter Cores due to Black-Hole Wandering"
arXiv:2607.00349 · 2026-07-01 · arXiv non-exclusive · independent analysis · 1 min
New simulations show black holes can't steadily feed on gas in galactic centers due to random wandering.

Just a few hundred million years after the Big Bang, quasars were already blazing — the cores of galaxies harboring black holes with billions of solar masses. The puzzle of their rapid growth remains unsolved. One hypothesis invokes a special kind of dark matter made of ultralight particles called axions, which behaves like a wave. It forms a dense knot at the galaxy's center, which, it seemed, would gravitationally pull in gas like a funnel.

But new simulations shatter this picture. The knot doesn't stay put: it quivers and shifts, and the hungry black hole tags along. Feeding becomes like trying to drink from a glass that's constantly being whisked away — sips of gas are rare and chaotic. Often the black hole leaves the dense region, and sometimes it's flung to the galaxy's outskirts, where the gas density is hundreds of times lower, and growth grinds to a halt.

Such a 'rogue' doesn't bulk up. Only intermediate-mass black holes might see a slight boost. So, fuzzy dark matter isn't the 'super-pump' that inflated ancient active galactic nuclei. The mystery endures: either a different type of hidden mass, or other feeding mechanisms. Perhaps the key lies in the properties of the first quasars, visible today at enormous distances.

In fact, the central clump of dark matter is a giant standing wave that forever quivers and drags the black hole across the galaxy.

\dot{M}_{\rm target} = 4\pi\lambda\frac{(G M_{\rm BH})^2\rho_\infty}{(c_s^2+v_{\rm rel}^2)^{3/2}}
Shows how black hole mass, gas density, and relative velocity determine the absorption rate.
\rho_{\rm sol}(r) = \rho_0\left[1+0.091\left(\frac{r}{r_c}\right)^2\right]^{-8}
Describes how soliton density gradually falls from the center, where it is maximum, to the periphery.
Scientists
Alan GuthAlexander FriedmannAndrei LindeGeorges LemaîtreJames PeeblesStephen Hawking
Concepts
supermassive black hole growth supermassive black hole nuclear reaction mass gap accretion disk wind dark matter core formation fuzzy dark matter accretion rate mass inflation wave amplification active galactic nucleus supermassive black hole formation black hole accretion