ArXiv TLDR

Calculation of a regularized Teukolsky Green function in Schwarzschild spacetime

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2604.21219

David Q. Aruquipa, Marc Casals, Brien C. Nolan

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TLDR

Exact separable form of the Teukolsky Green function in Schwarzschild spacetime improves gravitational perturbation analysis.

Key contributions

  • Derives exact Hadamard form factors for Teukolsky equation's retarded Green function.
  • Uses conformal spacetime to separate singular part into angular and radial components.
  • Calculates explicit angular factors linking geodesics, spin harmonics, and Euler angles.
  • Computes multipolar modes for electromagnetic and gravitational perturbations.

Why it matters

This paper refines the calculation of the Teukolsky Green function in Schwarzschild spacetime, crucial for modeling gravitational perturbations. Its exact separable form aids precise analysis near coincidence points, enhancing gravitational wave and black hole studies.

Original Abstract

We obtain exact expressions for various factors involved in the Hadamard form of the retarded Green function for the (Bardeen-Press-)Teukolsky equation on Schwarzschild spacetime. We use these to improve on previous results for the calculation of this Green function. We work in a spacetime $\mathcal{M}_2\times\mathbb{S}^2$ conformal to Schwarzschild, in which the metric takes a direct product form. This allows us to derive a separable form for the direct (i.e., singular) part of the Hadamard form of the retarded Green function. The angular factor in this quantity is calculated explicitly. This shows an interesting interplay between geodesics of $\mathbb{S}^2$, spin-weighted spherical harmonics, and Euler angles. The $\mathcal{M}_2$ factor equates to a spin-dependent factor that satisfies a transport equation along geodesics, times the square root of the van Vleck determinant. Both terms are calculated in an exact form for constant radius orbits (which includes the cases of circular timelike geodesics and static worldlines of Schwarzschild spacetime). This separable form also allows us to obtain the multipolar $\ell$-modes of the direct part for electromagnetic and gravitational field perturbations. We then use these $\ell$-modes to calculate, in the gravitational case, the retarded Green function minus its direct part: this is a better representation in practise of the retarded Green function for points near coincidence.

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