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Assessing the Energetics of Spinning Binary Black Hole Systems

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arxiv 1712.06533 v1 pith:Z2Q34VNY submitted 2017-12-18 gr-qc

classification gr-qc
keywords bindingenergysystemsapproximantsbinaryblackdynamicsextract
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abstract

In this work we study the dynamics of spinning binary black hole systems in the strong field regime. For this purpose we extract from numerical relativity simulations the binding energy, specific orbital angular momentum, and gauge-invariant orbital frequency. The goal of our work is threefold: First, we extract the individual spin contributions to the binding energy, in particular the spin-orbit, spin-spin, and cubic-in-spin terms. Second, we compare our results with predictions from waveform models and find that while post-Newtonian approximants are not capable of representing the dynamics during the last few orbits before merger, there is good agreement between our data and effective-one-body approximants as well as the numerical relativity surrogate models. Finally, we present phenomenological representations for the binding energy for non-spinning systems with mass ratios up to $q = 10$ and for the spin-orbit interaction for mass ratios up to $q = 8$ obtaining accuracies of $\lesssim 0.1\%$ and $\lesssim 6\%$, respectively.

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Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Kerr Soft Dressing and the $w_{1+\infty}$ Frame Algebra at Null Infinity

    hep-th 2026-07 conditional novelty 7.0 of 10

    The Kerr soft exponent generates a parity-alternating hierarchy of null-infinity frame generators—displacement memory at s=0, spin memory at s=1, and higher moments alternating by Kerr multipole parity—realized as the...

  2. Binary Black Hole Phase Space Discovers the Signature of Pair Instability Supernovae Mass Gap

    astro-ph.HE 2025-09 reject novelty 4.0 of 10

    Applying a phase-space overlap method to GWTC-4, the paper claims first-generation black holes are truncated near 45.5 solar masses, but the cutoff follows from the assumed exponential mass prior rather than from the data.

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