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Leading effective field theory corrections to the Kerr metric at all spins

Pedro G. S. Fernandes

Abstract

The leading corrections to General Relativity can be parametrized by higher-derivative interactions in a low-energy effective field theory, in a way that is general and agnostic to the precise UV completion of gravity. Using pseudospectral methods, we compute the leading-order corrections to the Kerr metric across the entire range of sub-extremal values of spin and analyse their impact on physical quantities. We find that near-extremal black holes are most affected by the higher-derivative corrections, making them especially sensitive probes of new physics. A dataset of solutions and the code used to produce them are publicly available.

Leading effective field theory corrections to the Kerr metric at all spins

Abstract

The leading corrections to General Relativity can be parametrized by higher-derivative interactions in a low-energy effective field theory, in a way that is general and agnostic to the precise UV completion of gravity. Using pseudospectral methods, we compute the leading-order corrections to the Kerr metric across the entire range of sub-extremal values of spin and analyse their impact on physical quantities. We find that near-extremal black holes are most affected by the higher-derivative corrections, making them especially sensitive probes of new physics. A dataset of solutions and the code used to produce them are publicly available.

Paper Structure

This paper contains 13 equations, 2 figures.

Figures (2)

  • Figure 1: Absolute difference between the numerical and analytic values of $\kappa_{(4)}$ (top) and $\Omega_{H,(4)}$ (bottom) for both parity sectors. The numerical values were obtained using resolutions $(N_x, N_y) = (50,16)$ for $a/M < 0.65$, $(N_x, N_y) = (60,24)$ for $0.65 \leq a/M < 0.999$, and $(N_x, N_y) = (64,28)$ for $a/M = 0.999$. In the parity-odd case, the analytic values of these quantities are identically zero.
  • Figure 2: Corrections to the perimetral location (top) and orbital frequency at the light ring (bottom) for spin values up to $a/M=0.99$.