How a Star's Insides Bend Its Path ✎ express

Original: "A Rigorous Jacobi-Metric Approach to the Gauss-Bonnet Lensing of Spinning Particles: Extension to Quadrupole Order"
· Hoang Van Quyet
arXiv:2603.20657 · 2026-03-21 · arXiv non-exclusive · independent analysis · 1 min
Spin and shape of a celestial body alter its trajectory near a black hole.

📄 Showing the "Simple" version — "Advanced" is not ready yet. Add it to favorites to help prioritize it.

A heavy spinning top launched near a black hole doesn't follow the curve that textbooks draw. Its own rotation and oblateness, like a pumpkin squashed at the poles, make the trajectory wobble. In a new study, this wobbling path has been calculated more precisely than ever before.

Usually, a small body in a black hole's field is treated as a point — without size or spin. But real neutron stars or black hole candidates spin rapidly and become noticeably deformed. Accounting for this deformation (the quadrupole moment) adds an extra bend to the body's path. The authors derived a formula: the correction to the deflection angle grows with the square of the spin and inversely with the cube of the impact parameter — the distance at which the body passes by the black hole.

The closer to the black hole and the faster the spin, the stronger the influence of the body's internal structure on its path.

The formula is derived not for an abstract geodesic but for a real trajectory, including the force that arises from the interaction of spin with spacetime curvature. This could allow future observations of the deflection of light or matter to reveal what lies inside, just as the wobble of a spinning top hints at its contents.

If Earth spun as fast as some neutron stars, its equatorial radius would be noticeably larger than its polar radius, and satellites in low orbits would feel that oblateness.

\delta\alpha \propto \frac{C_Q s^2 M}{b^3}
The correction to the deflection angle is proportional to the quadrupole moment constant C_Q, the square of the spin s, the black hole mass M, and inversely proportional to the cube of the impact parameter b.
Scientists
Stephen HawkingJacob BekensteinFritz ZwickyBernhard RiemannJoseph WeberKarl Schwarzschild
Concepts
geodesic equation quadrupole radiation formula classical gravity general relativity gravitational field spin curvature coupling Law of Universal Gravitation gravitational pull light deflection Birkhoff's theorem fq gravity Klein-Gordon equation dark matter lensing quadrupole moment strong lensing Kepler's third law schwarzschild metric metric Gauss's theorem supergravity