Gravitational Acceleration of Dark Matter by Black Holes at the Center of the Milky Way ✛ ✎ ✦

Original: "Boosted Dark Matter from Sagittarius A$$^\star$$"
· Javier F. Acevedo, Adam Ritz
arXiv:2606.30724 · 2026-06-29 · arXiv non-exclusive · independent analysis · 4 min
Stellar-mass black holes near Sagittarius A* can accelerate dark matter particles to speeds that allow their detection in detectors.

Context

The detection of dark matter, first proposed by Fritz Zwicky to explain the motion of galaxies in clusters, remains one of the key challenges of modern physics. Although direct detection experiments like LZ, XENONnT, and DarkSide-50 have achieved impressive sensitivity, their ability to register light dark matter is limited by the low velocities of particles in the galactic halo. However, it has recently been realized that binary black holes can serve as natural accelerators, boosting dark matter via gravitational slingshot. Of particular interest is the nuclear star cluster at the center of our Galaxy, where Sagittarius A*, a supermassive black hole with a mass of about 4 million solar masses, is surrounded by a swarm of tens of thousands of stellar-mass black holes. The high density of dark matter and extreme gravitational potential make this region an ideal factory of fast dark matter. Detailed observations by Vera Rubin and others confirmed the presence of hidden mass in galaxies.

Methods

To estimate the flux of accelerated dark matter, the authors applied numerical simulation of the restricted three-body problem using the Verlet algorithm. In each simulation, a dark matter particle was injected into the sphere of influence of a system of two black holes, and its trajectory was calculated taking into account Newtonian gravity and energy conservation. The orbits of the black holes were prescribed based on a power-law Bahcall–Wolf profile, consistent with observational data on star formation and metallicity in the Galactic center, and the population was modeled taking into account stellar evolution. The distribution of dark matter was described by a Navarro–Frenk–White profile with a correction for gravitational focusing by Sagittarius A*. To account for all possible initial conditions, the phase space of orbits was binned, and for each bin the differential ejection spectrum was calculated. The use of angular momentum conservation and Jeans theorem allowed linking the orbital distribution with the density of black holes.

Results

The results of the simulation showed that black holes in the nuclear star cluster can eject dark matter at speeds up to 25,000 km/s, with the main contribution to the high-energy tail coming from only a few tens of black holes on short-period orbits. The integral ejection spectrum exceeds the flux from any other known galactic sources of accelerated dark matter. Remarkably, even under conservative assumptions about the density profile of dark matter, large-volume detectors gain sensitivity to masses down to 60 MeV for elastic scattering, and for inelastic processes with masses on the order of TeV, splittings up to 9 MeV become accessible. Calculations also demonstrate that a single intermediate-mass black hole on a close orbit can produce a comparable effect.

Implications

This result means that dark matter can be detected in experiments that were not originally optimized for low masses. Black holes at the center of the Galaxy become a new tool of particle astrophysics, independent of specific interaction models. Detecting a signal from such a flux would not only confirm the existence of dark matter, but also probe the distribution of black holes near the supermassive black hole and the structure of the galactic center.

Future development

In the future, with the commissioning of new gravitational-wave observatories, such as LISA, independent mapping of the population of black holes near Sagittarius A* will become possible. This will allow refining predictions of accelerated dark matter fluxes and possibly discovering correlations between gravitational-wave events and signals in dark matter detectors. Additionally, improving detectors and scaling to multi-ton scales will open the way to studying a wide class of inelastic dark matter models.

Impact

The discovery will impact both particle physics, providing a new way to search for dark matter without being tied to specific masses and interaction constants, and the dynamics of galaxies, highlighting the role of nuclear clusters in redistributing dark matter.

Next steps

The next step is to include in the calculations bound states of dark matter around Sagittarius A* and to account for mass segregation effects, which could further increase the flux of fast particles. Also planned is a detailed study of the possibility of registering such events with neutrino observatories.

Key open problems

This work is directly connected to unresolved questions about the nature of dark matter, the distribution of black holes at the center of the Galaxy, and the mechanisms of formation of galactic nuclei. The success of the proposed approach could shed light on the long-standing problem of "cusps" in the density profiles of dark matter.

The knowledge machine's view

This section is addressed to the author of the paper and their colleagues. Neighbouring works were found by meaning-based search across our archive, not by word overlap. We do not review: we show the field around the work.

What the work does

The study examines how stellar-mass black holes in the Milky Way's nuclear star cluster can gravitationally accelerate dark matter particles. Using numerical simulations of the restricted three-body problem and accounting for orbital distributions, it is found that the velocities of ejected dark matter reach 25,000 km/s, and the main contribution to the high-energy tail comes from a few dozen black holes.

Where its strength is

The strength of the work lies in its specific quantitative estimate of the flux of accelerated dark matter from compact objects at the Galactic center, linking the dynamics of the nuclear cluster to the possibilities of direct detection.

Where it could go next

Worth trying

  • Test a combined treatment of particle acceleration from both binary black holes and the supermassive black hole.
  • Investigate how a wind from the central black hole changes the dark matter density in the acceleration zone.
  • Compare predicted spectra with constraints from gamma-ray observations of the Galactic center.

Why this may matter

If fast dark matter indeed exists, it would open a new window for direct detection even at low particle masses, and also allow linking the dynamics of the Galactic center to signals in terrestrial experiments.

Although at the center of the Galaxy the density of dark matter can be thousands of times higher than locally, the accelerated particles reaching Earth originate from an infinitesimally small fraction — only those that found themselves "on the wrong orbit" too close to black holes.

In the movie "Interstellar," the heroes use a gravitational maneuver around the black hole Gargantua to save fuel. In reality, black holes at the center of our Galaxy can act as giant slingshots, accelerating dark matter to near-light speeds.

\Delta\varepsilon \approx 2 v_i u_{M_2}
Δε is the change in specific energy, v_i is the initial particle velocity, u_{M2} is the orbital velocity of the black hole
v_{\chi}^{(\mathrm{min})} \approx \frac{1}{\sqrt{2 m_N E_R}} \left( \frac{E_R m_N}{\mu_{\chi N}} + \delta \right)
vχ(min) is the minimum dark matter velocity to excite a recoil nucleus with energy E_R, m_N is the nucleus mass, μχN is the reduced mass, δ is the mass difference between states

Key numbers

  • maximum ejection velocity: ~25,000 km/s
  • number of black holes in the nuclear cluster: ~2.5×105
  • distance from Earth to the Galactic center: ~8.2 kpc
  • achieved dark matter mass for xenon detectors: ~60 MeV
  • maximum mass splitting for inelastic scattering: up to 9 MeV
Scientists
Fritz ZwickyStephen HawkingJacob BekensteinVera RubinMargaret BurbidgeMaarten Schmidt
Concepts
milky way central black hole galactic center dark star black hole neutrino source gravitational atom galactic dust winds dark energy active galaxy cosmic particle acceleration accretion disk wind milky way microquasar blazar m87 cosmic accelerator expansion of the universe ultra fast outflow donor star hills mechanism gw190814