A Dark Matter Veil: How It Bends a Star's Light ✛ ✎

Original: "Weak gravitational lensing by a dark-matter-admixed neutron star: a self-consistent two-fluid halo and the Gauss--Bonnet deflection angle"
· Yashmitha Kumaran, Ilídio Lopes
arXiv:2608.25587v1 · 2026-08-26 · arXiv non-exclusive · independent analysis · 1 min
An invisible halo around a neutron star makes light bend less, and this weakening reveals how much dark matter lies within.

A light ray flying past a massive body bends slightly. For a neutron star, this bending is usually assumed to be the same as for a point with the same mass. But if the star is surrounded by an invisible cloud of dark matter, light passing through that cloud is deflected more weakly. The reason is simple: the cloud is spread out in space, and the light only feels the part of it that lies within a cylinder around the ray. The farther from the center, the less mass there is, and the weaker the bend.

For a star with a dark matter fraction of 0.35 and a cloud radius of 30 km, the light deflection at the inner edge is one-third less than if all the mass were at a single point.

The scientists built a model of a star where ordinary matter and dark matter coexist as two fluids that interact only through gravity. For light dark matter particles, pressure puffs them into a cloud beyond the visible surface. They then computed the light deflection angle using a geometric theorem. It turned out that the shape of the deflection weakening depends on the dark matter fraction and the cloud size. This makes it possible to distinguish dark matter from uncertainties in the properties of ordinary matter.

The light deflection angle of a neutron star with a dark halo at an impact parameter equal to the halo radius is about 16 degrees, which is much larger than the Sun's deflection of 1.75 arcseconds.

\hat{\alpha}(b) \simeq \frac{4G}{c^2 b} M_{\rm cyl}(b)
The deflection is proportional to the cylindrical mass within the impact parameter b, not the total mass of the star
M_{\rm cyl}(b) = M_B + 4\pi \int_{R_B}^{R_\chi} \rho_\chi(r) W(r,b) r^2 dr
The mass of the baryonic core plus the contribution of the dark halo, weighted by the projection function W(r,b)
W(r,b) = \begin{cases} 1, & r \le b \\ 1 - \sqrt{1 - b^2/r^2}, & r > b \end{cases}
Determines what fraction of the shell's mass falls inside the cylinder
Scientists
Fritz ZwickyVera RubinSubrahmanyan ChandrasekharJocelyn Bell BurnellWolfgang PauliAdam Riess
Concepts
weak lensing dark matter lensing gravitational microlensing dark matter deficient dwarf galaxies compactness collapse neutron star composition galactic halo galactic halo composition compact object light deflection boson star stellar remnant Birkhoff's theorem stellar mass black hole dust obscuration neural network galaxy mapping density profile gravitational collapse fritz zwicky