Multipole moments on the common horizon in a binary-black-hole simulation

被引:5
|
作者
Chen, Yitian [1 ]
Kumar, Prayush [1 ,2 ]
Khera, Neev [3 ,4 ]
Deppe, Nils [5 ]
Dhani, Arnab [3 ,4 ]
Boyle, Michael [1 ]
Giesler, Matthew [1 ]
Kidder, Lawrence E. [1 ]
Pfeiffer, Harald P. [6 ]
Scheel, Mark A. [5 ]
Teukolsky, Saul A. [1 ,5 ]
机构
[1] Cornell Univ, Cornell Ctr Astrophys & Planetary Sci, Ithaca, NY 14853 USA
[2] Tata Inst Fundamental Res, Int Ctr Theoret Sci, Bangalore 560089, India
[3] Penn State, Inst Gravitat & Cosmos, University Pk, PA 16802 USA
[4] Penn State, Phys Dept, University Pk, PA 16802 USA
[5] CALTECH, Theoret Astrophys 350 17, Pasadena, CA 91125 USA
[6] Max Planck Inst Gravitat Phys, Albert Einstein Inst, Muhlenberg 1, D-14476 Potsdam, Germany
关键词
MODE-STABILITY; PERTURBATIONS; EQUATIONS; FINDER;
D O I
10.1103/PhysRevD.106.124045
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
We construct the covariantly defined multipole moments on the common horizon of an equal-mass, nonspinning, quasicircular binary-black-hole system. We see a strong correlation between these multipole moments and the gravitational waveform. We find that the multipole moments are well described by the fundamental quasinormal modes at sufficiently late times. For each nonzero multipole moment with l <= 6, at least two fundamental quasinormal modes of different l are detectable in the best model. These models provide faithful estimates of the true mass and spin of the remnant black hole. We also show that by including overtones, the l = m = 2 mass multipole moment admits an excellent quasinormal-mode description at all times after the merger. This demonstrates the perhaps surprising power of perturbation theory near the merger.
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页数:23
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