Galaxies without dark matter: a sieve for the invisible ✛

Original: "Dark Matter Deficient Galaxies as Probes of Dark Matter"
· Oem Trivedi, Abraham Loeb
arXiv:2607.26085v1 · 2026-07-27 · CC BY 4.0 · 3 min
Deficient galaxies act as a sieve, sifting dark matter, so we learn how strongly it clings to ordinary matter.

In the galaxy NGC 1052 DF2, stars move at only 8 kilometers per second, as if there were no invisible mass around. For comparison: in our Milky Way, outlying stars accelerate to 200 kilometers per second, held by a massive dark matter halo. Fritz Zwicky suspected its existence as early as the 1930s, and Vera Rubin confirmed it in the 1970s: without an invisible framework, galaxies would fly apart. But here — a star cluster deprived of its usual support. It is precisely such 'empty' systems that become a sieve, sifting dark matter through ordinary matter.

Galaxy collisions are a grand cosmic shake-up. Ordinary matter clings, rubs, heats up, and slows down, while dark matter glides past, barely noticing obstacles. Imagine a handful of sand and a pinch of metal dust thrown into water: the sand immediately gets wet and sinks, while the dust, if water-repellent, rushes on. On a galactic scale, these 'washings' leave behind objects almost devoid of dark matter. Their existence signals how weakly it interacts with baryons.

Astrophysicists have developed a quantitative criterion for such a sieve. They ask: what fraction of dark matter remains in the resulting galaxy after a collision? If that fraction is below a threshold (say, 1%), the mixture has truly separated. The condition is expressed as an inequality, where the main variables are the intensity of 'stickiness' (momentum-transfer cross section) and the fraction of the interacting component. The finer the sieve, the less impurity it can retain.

Stickiness limit: for constant interaction, the cross section is limited to 0.50 cm²/g. If the effect weakens with speed (as for n=4), the upper bound tightens to 2.3×10⁻⁶ cm²/g — millions of times stricter.

Not everything boils down to a head-on collision. Dark matter could cool and settle into a flat disk, such models are called dissipative. For the shell loss to succeed, the cooling fraction must be minuscule: less than a percent, otherwise matter won't separate. Another scenario is an ultralight axion field forming quantum clumps. They are torn apart by tidal forces if the escape velocity from the system is about 96 times greater than the drift speed. This picks out a narrow mass window: roughly 10⁻²³–10⁻²² eV. Each such option is its own cell in the galactic sieve.

Invisible masses: the ultralight particles discussed here are 10²⁸ times lighter than an electron. Like a speck on the cosmic scales, but their wave properties are felt over thousands of light-years.

The slow stars of NGC 1052 DF2 are not an anomaly but evidence of a giant sieve at work. Each such galaxy becomes a tool that probes the properties of invisible matter at the microscale. And the more of them future surveys like LSST find, the more precisely we will tune this sieve. What began as a mystery of an almost weightless star cluster turns into a key to one of the main problems in physics.

In the galaxy NGC 1052 DF2, the stellar velocity dispersion is only about 8 km/s, as if all the mass were provided by the stars themselves, with no dark matter halo.

f_{\mathrm{int}}(1 - e^{-D_{\chi b}}) + (1 - f_{\mathrm{int}}) f_{\mathrm{grav}} \le \delta
The inequality links the fraction of interacting dark matter f_int, the drag depth D_χb, and the gravitational capture efficiency f_grav to the required threshold δ.
\frac{\sigma_0}{m_\chi + m_b} \le \frac{-\ln(1-\delta)}{\Sigma_b} \left(\frac{v_0}{v_{\mathrm{col}}}\right)^n
Upper limit on the cross-section normalization σ₀/(m_χ+m_b) as a function of the exponent n, the baryon column density Σ_b, and the velocity ratio v₀/v_col.
Scientists
Fritz ZwickyRashid Alievich SunyaevAugustin-Louis CauchyChristiaan HuygensEmmy NoetherIsaac Newton
Concepts
dark matter deficient dwarf galaxies dark matter detection axion detection axion galaxy formation mass ratio mass distribution neural network galaxy mapping dust extinction metal poor galactic halo composition dust obscuration rare event search hidden particle decay weak lensing black hole formation mechanism galactic halo gravitational lensing analysis alternative gravity tests high redshift galaxies