Quasi-normal modes of slowly-rotating Johannsen black holes

Abstract The detection of gravitational waves with ground-based laser interferometers has opened a new window to test and constrain General Relativity (GR) in the strong, dynamical, and non-linear regime. In this paper, we follow an agnostic approach and we study the quasi-normal modes of gravitational perturbations of Johannsen black holes under the assumptions of the validity of the Einstein Equations and of low values of the black hole spin parameter and deformation parameters. We find that the deformation parameter $$\alpha _{13}$$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msub> <mml:mi>α</mml:mi> <mml:mn>13</mml:mn> </mml:msub> </mml:math> has a stronger impact on the quasi-normal modes than the other leading order deformation parameters ( $$\alpha _{22}$$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msub> <mml:mi>α</mml:mi> <mml:mn>22</mml:mn> </mml:msub> </mml:math> , $$\alpha _{52}$$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msub> <mml:mi>α</mml:mi> <mml:mn>52</mml:mn> </mml:msub> </mml:math> , and $$\epsilon _{3}$$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msub> <mml:mi>ϵ</mml:mi> <mml:mn>3</mml:mn> </mml:msub> </mml:math> ). We derive a fitting formula for the fundamental modes with $$l=2$$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mrow> <mml:mi>l</mml:mi> <mml:mo>=</mml:mo> <mml:mn>2</mml:mn> </mml:mrow> </mml:math> and $$l=3$$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mrow> <mml:mi>l</mml:mi> <mml:mo>=</mml:mo> <mml:mn>3</mml:mn> </mml:mrow> </mml:math> for the deformation parameter $$\alpha _{13}$$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msub> <mml:mi>α</mml:mi> <mml:mn>13</mml:mn> </mml:msub> </mml:math> valid in the slow rotation approximation ( $$a_* &lt; 0.4$$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mrow> <mml:mmultiscripts> <mml:mi>a</mml:mi> <mml:mrow> <mml:mrow/> <mml:mo>∗</mml:mo> </mml:mrow> <mml:mrow/> </mml:mmultiscripts> <mml:mo>&lt;</mml:mo> <mml:mn>0.4</mml:mn> </mml:mrow> </mml:math> ). Finally, we constrain $$\alpha _{13}$$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msub> <mml:mi>α</mml:mi> <mml:mn>13</mml:mn> </mml:msub> </mml:math> from the event GW170104; within our analysis, we find that the data of GW170104 are consistent with the predictions of GR.

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Publication Details

Journal
The European Physical Journal C
Published
2025-04-16
DOI
https://doi.org/10.1140/epjc/s10052-025-14118-9
Primary Topic
Pulsars and Gravitational Waves Research
Type
article
Field-Weighted Citation Impact
0.00

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article

Quasi-normal modes of slowly-rotating Johannsen black holes

Cosimo Bambi, Swarnim Shashank, Yuhao Guo
The European Physical Journal C
Pulsars and Gravitational Waves Research
article

Quasi-normal modes of slowly-rotating Johannsen black holes

Cosimo Bambi, Swarnim Shashank, Yuhao Guo
article en

Abstract

Abstract The detection of gravitational waves with ground-based laser interferometers has opened a new window to test and constrain General Relativity (GR) in the strong, dynamical, and non-linear regime. In this paper, we follow an agnostic approach and we study the quasi-normal modes of gravitational perturbations of Johannsen black holes under the assumptions of the validity of the Einstein Equations and of low values of the black hole spin parameter and deformation parameters. We find that the deformation parameter $$\alpha _{13}$$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msub> <mml:mi>α</mml:mi> <mml:mn>13</mml:mn> </mml:msub> </mml:math> has a stronger impact on the quasi-normal modes than the other leading order deformation parameters ( $$\alpha _{22}$$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msub> <mml:mi>α</mml:mi> <mml:mn>22</mml:mn> </mml:msub> </mml:math> , $$\alpha _{52}$$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msub> <mml:mi>α</mml:mi> <mml:mn>52</mml:mn> </mml:msub> </mml:math> , and $$\epsilon _{3}$$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msub> <mml:mi>ϵ</mml:mi> <mml:mn>3</mml:mn> </mml:msub> </mml:math> ). We derive a fitting formula for the fundamental modes with $$l=2$$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mrow> <mml:mi>l</mml:mi> <mml:mo>=</mml:mo> <mml:mn>2</mml:mn> </mml:mrow> </mml:math> and $$l=3$$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mrow> <mml:mi>l</mml:mi> <mml:mo>=</mml:mo> <mml:mn>3</mml:mn> </mml:mrow> </mml:math> for the deformation parameter $$\alpha _{13}$$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msub> <mml:mi>α</mml:mi> <mml:mn>13</mml:mn> </mml:msub> </mml:math> valid in the slow rotation approximation ( $$a_* &lt; 0.4$$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mrow> <mml:mmultiscripts> <mml:mi>a</mml:mi> <mml:mrow> <mml:mrow/> <mml:mo>∗</mml:mo> </mml:mrow> <mml:mrow/> </mml:mmultiscripts> <mml:mo>&lt;</mml:mo> <mml:mn>0.4</mml:mn> </mml:mrow> </mml:math> ). Finally, we constrain $$\alpha _{13}$$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msub> <mml:mi>α</mml:mi> <mml:mn>13</mml:mn> </mml:msub> </mml:math> from the event GW170104; within our analysis, we find that the data of GW170104 are consistent with the predictions of GR.

The European Physical Journal CVol. 85(4)
Fudan University (CN), New Uzbekistan University (UZ), National University of Uzbekistan (UZ)
Natural Science Foundation of Shanghai, National Natural Science Foundation of China
Openalex Percentile: Top 94%
Pulsars and Gravitational Waves Research
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