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Interplay between numerical relativity and perturbation theory : finite size effects
General Relativity and Quantum Cosmology · Submitted 14 Jun 2023
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We demonstrate that by considering the secondary as a finite size object, the BHPT waveforms closely match NR waveforms.
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The abstract, sentence by sentence
We investigate the interplay between numerical relativity (NR) and point-particle black hole perturbation theory (ppBHPT) in the comparable mass ratio regime. In the ppBHPT framework, the secondary black hole is treated as a point particle, neglecting its finite size. Our study focuses on addressing the missing finite size effect in the ppBHPT framework and proposing a method for incorporating the size of the secondary into the perturbation theory framework. We demonstrate that by considering the secondary as a finite size object, the BHPT waveforms closely match NR waveforms. Additionally, we revisit the $\alpha$-$\beta$ scaling technique, which was previously introduced by Islam et al, as a means to effectively match ppBHPT waveforms to NR waveforms. We further analyze the scaling procedure and decompose it into different components, attributing them to various effects, including the corrections arising from the finite size of the secondary black hole.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We investigate the interplay between numerical relativity (NR) and point-particle black hole perturbation theory (ppBHPT) in the comparable mass ratio regime. | contribution 0.77 | 0.87 | 0.04 | asserted 0.79 |
| s1 | In the ppBHPT framework, the secondary black hole is treated as a point particle, neglecting its finite size. | background 0.95 | 0.09 | 0.03 | asserted 1.00 |
| s2 | Our study focuses on addressing the missing finite size effect in the ppBHPT framework and proposing a method for incorporating the size of the secondary into the perturbation theory framework. | contribution 0.90 | 0.77 | 0.14 | asserted 0.87 |
| s3 | We demonstrate that by considering the secondary as a finite size object, the BHPT waveforms closely match NR waveforms. | result 1.00 | 0.94 | 0.70 | asserted 1.00 |
| s4 | Additionally, we revisit the $\alpha$-$\beta$ scaling technique, which was previously introduced by Islam et al, as a means to effectively match ppBHPT waveforms to NR waveforms. | contribution 0.55 | 0.60 | 0.06 | asserted 0.90 |
| s5 | We further analyze the scaling procedure and decompose it into different components, attributing them to various effects, including the corrections arising from the finite size of the secondary black hole. | contribution 0.53 | 0.91 | 0.09 | asserted 1.00 |
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The paper
Original abstract
We investigate the interplay between numerical relativity (NR) and point-particle black hole perturbation theory (ppBHPT) in the comparable mass ratio regime. In the ppBHPT framework, the secondary black hole is treated as a point particle, neglecting its finite size. Our study focuses on addressing the missing finite size effect in the ppBHPT framework and proposing a method for incorporating the size of the secondary into the perturbation theory framework. We demonstrate that by considering the secondary as a finite size object, the BHPT waveforms closely match NR waveforms. Additionally, we revisit the $\alpha$-$\beta$ scaling technique, which was previously introduced by Islam et al, as a means to effectively match ppBHPT waveforms to NR waveforms. We further analyze the scaling procedure and decompose it into different components, attributing them to various effects, including the corrections arising from the finite size of the secondary black hole.
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References
How the literature uses it
5 arXiv papers cite this in 20 sentences
Papers citing it · 13 sentences without a confident label
Compares with it 1 paper
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Interestingly, the determined value of $α_ℱ^median$ closely aligns with the estimated correction parameter $α_size,ℓ=2(=0.958)$ that accounts for the missing finite size effect of the secondary black hole in BHPT framework [ref] .
Mapping between black-hole perturbation theory and numerical relativity: gravitational-wave energy flux · Estimating $α_ℱ$ and $β_ℱ$ parameters · 0.81
Cites it as support 2 papers
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Further analysis provides evidence that the calibration parameters can be attributed to the absence of finite size effects within the ppBHPT framework [ref] .
On the approximate relation between black-hole perturbation theory and numerical relativity · Introduction · 0.97
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Assuming that this feature correctly extrapolates to the comparable masses case (as supported by many similar examples in the two-body problem, see e.g. Refs. [ref] ), simulations with a short inspiral should be sufficient to preserve the $A_tail$ scaling with the eccentricity.
Inspiral-inherited ringdown tails · Future developments · 0.99
Cites it as background 1 paper
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These works involve developing a fully second-order self-force waveforms for non-spinning binary black holes [ref] , discovery of a simple underlying relation named the $α$-$β$ mapping between BHPT and NR waveforms in the comparable mass regime [ref] , building NR-tuned BHPT waveform model for comparable to extreme mass ratio binary [ref] and performing the first set of high mass ratio NR simulations up to $∼q=1000$ [ref] .
Mapping between black-hole perturbation theory and numerical relativity: gravitational-wave energy flux · Introduction · 0.93
What it cites · 4 sentences without a confident label
Uses the method or tool of 14 papers
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To generate the NR waveforms, we utilize the waveform model [ref] , which is a surrogate waveform trained on NR data hybridized with post-Newtonian-corrected effective-one-body inspirals.
Surrogate model of hybridized numerical relativity binary black hole waveforms · Understanding the effect of finite size in ppBHPT waveforms · 0.97
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Once the trajectory of the perturbing compact body is fully specified, we solve the inhomogeneous Teukolsky equation in the time-domain while feeding the trajectory information into the particle source-term of the equation [ref] .
Binary black hole merger gravitational waves and recoil in the large mass ratio limit · Point-particle perturbation theory · 0.95
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Once the trajectory of the perturbing compact body is fully specified, we solve the inhomogeneous Teukolsky equation in the time-domain while feeding the trajectory information into the particle source-term of the equation [ref] .
A GPU-accelerated mixed-precision WENO method for extremal black hole and gravitational wave physics computations · Point-particle perturbation theory · 0.95
Cites as background 37 papers
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These advancements include the development of the surrogate model [ref] and a fully relativistic second-order self-force model [ref] , as well as the expansion of numerical relativity (NR) techniques to simulate BBH mergers with higher mass ratios [ref] .
Study of the Intermediate Mass Ratio Black Hole Binary Merger up to 1000:1 with Numerical Relativity · Introduction · 0.88
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These advancements include the development of the surrogate model [ref] and a fully relativistic second-order self-force model [ref] , as well as the expansion of numerical relativity (NR) techniques to simulate BBH mergers with higher mass ratios [ref] .
Targeted large mass ratio numerical relativity surrogate waveform model for GW190814 · Introduction · 0.88
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These advancements include the development of the surrogate model [ref] and a fully relativistic second-order self-force model [ref] , as well as the expansion of numerical relativity (NR) techniques to simulate BBH mergers with higher mass ratios [ref] .
Gravitational waveforms for compact binaries from second-order self-force theory · Introduction · 0.88
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