New effective precession spin for modeling multimodal gravitational waveforms in the strong-field regime

L. Thomas, P. Schmidt, G. Pratten
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引用次数: 6

Abstract

Accurately modelling the complete gravitational-wave signal from precessing binary black holes through the late inspiral, merger and ringdown remains a challenging problem. The lack of analytic solutions for the precession dynamics of generic double-spin systems, and the high dimensionality of the problem, obfuscate the incorporation of strong-field spin-precession information into semi-analytic waveform models used in gravitational-wave data analysis. Previously, an effective precession spin, $\chi_p$, was introduced to reduce the number of spin degrees of freedom. Here, we show that $\chi_p$ alone does not accurately reproduce higher-order multipolar modes, in particular the ones that carry strong imprints due to precession such as the $(2,1)$-mode. To improve the higher-mode content, and in particular to facilitate an accurate incorporation of precession effects in the strong-field regime into waveform models, we introduce a new dimensional reduction through an effective precession spin vector, $\vec{\chi}_\perp$, which takes into account precessing spin information from both black holes. We show that this adapted effective precession spin (i) mimics the precession dynamics of the fully precessing configuration remarkably well, (ii) captures the signature features of precession in higher-order modes, and (iii) reproduces the final state of the remnant black hole with high accuracy for the overwhelming majority of configurations. We demonstrate the efficacy of this two-dimensional precession spin in the strong-field regime, paving the path for meaningful calibration of the precessing sector of semi-analytic waveform models with a faithful representation of higher-order modes through merger and the remnant black hole spin.
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模拟强场下多模态引力波的新有效旋进
精确地模拟双黑洞在后期激发、合并和衰荡过程中产生的完整引力波信号仍然是一个具有挑战性的问题。一般双自旋系统进动动力学的解析解的缺乏,以及问题的高维性,使得将强场自旋进动信息纳入引力波数据分析中使用的半解析波形模型变得模糊。以前,引入了一个有效的进动自旋$\chi_p$来减少自旋自由度的数量。在这里,我们表明$\chi_p$本身并不能准确地再现高阶多极模态,特别是那些由于进动而携带强印记的模式,如$(2,1)$ -模态。为了提高高模含量,特别是为了将强场状态下的进动效应精确地整合到波形模型中,我们通过一个有效的进动自旋矢量$\vec{\chi}_\perp$引入了一个新的降维方法,该矢量考虑了来自两个黑洞的自旋信息。我们表明,这种适应的有效进动自旋(i)非常好地模拟了完全进动构型的进动动力学,(ii)捕获了高阶模式下进动的特征,(iii)高精度地再现了绝大多数构型的残余黑洞的最终状态。我们证明了这种二维进动自旋在强场域中的有效性,为通过合并和残余黑洞自旋忠实地表示高阶模式的半解析波形模型的进动部分的有意义的校准铺平了道路。
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