The Master Key to the Secrets of Spinning Black Holes ✛

Original: "Hidden simplicity in the scattering for neutron stars and black holes"
· Rafael Aoude, Andreas Helset
arXiv:2509.04425 · 2025-09-04 · CC BY 4.0 · 1 min
Scientists found a way to replace mountains of equations with a single action — taking a derivative of a generating function.

The focus is on a spinning black hole. Its gravity is so strong that it warps the space around it, altering the trajectory of everything passing by. Calculating such interactions with a neutron star, a superdense object the size of a city, required solving cumbersome equations. The authors of the paper came up with an elegant trick: they reduced all computations to a single generating function. This mathematical tool is like a universal dough: from it, by simple differentiation (like slicing), you instantly get any detail of the process — from the force of attraction to the star's deformation.

The black hole's tidal forces stretch the neutron star, and the new method allowed calculating this deformation without months-long computer simulations. Amazingly, the function contains all possible scenarios at once: it describes an encounter with any black hole, of any size and rotation speed: you just plug in the parameters.

This approach not only saves time but also helps more accurately predict elusive gravitational waves — ripples in spacetime that scientists have only recently begun to detect.

Generating functions were invented in the 18th century for coin change problems, and now they unlock the mysteries of black holes.

The stretching of a neutron star resembles scenes from 'Interstellar': the black hole Gargantua similarly deforms everything that approaches it.

G^{(L,k)}(a) = \int \hat{d}^D\ell_1 \cdots \hat{d}^D\ell_L \frac{1}{(2v_1\cdot\ell_1)\cdots(2v_1\cdot\ell_{1\cdots L})} \frac{1}{\ell_1^2\cdots\ell_L^2(q-\ell_{1\cdots L})^2} \exp[\ell_{1\cdots k}\cdot a]
Integral over L loop momenta with an exponential factor depending on the spin vector a; differentiation with respect to a yields tensor integrals.
c^{(L,k)}_{i,j} = \frac{2^{2i+j} (d(L+1-k))_i (dk)_{i+j}}{(dL)_i (d(L+1))_{2i+j}} \, {}_3F_2\left(\genfrac{}{}{0pt}{}{d(L+1-k)+i, \frac{1-j}{2}, -\frac{j}{2}}{dL+i, 1-dk-i-j}; 1\right)
The coefficients are expressed in terms of the hypergeometric function 3F2 and Pochhammer symbols; they determine the contribution of each spin order.
Scientists
Stephen HawkingJacob BekensteinFritz ZwickyBernhard RiemannJoseph WeberKarl Schwarzschild
Concepts
kerr black hole Penrose process effective spin black hole neutrino source kerr effect accretion disk wind torus spin rate neutron scattering Hawking radiation hawking radiation mechanism ringdown active galaxy gravastar kerr metric rotating black hole wald entropy neutron star dark matter dark matter lensing