Constructing effective one-body dynamics with numerical energy flux for intermediate-mass-ratio inspirals
被引:31
作者:
Han, Wen-Biao
论文数: 0引用数: 0
h-index: 0
机构:
Univ Roma La Sapienza, ICRANet, I-65122 Pescara, Italy
Univ Roma La Sapienza, Dept Phys, I-65122 Pescara, ItalyUniv Roma La Sapienza, ICRANet, I-65122 Pescara, Italy
Han, Wen-Biao
[1
,2
]
Cao, Zhoujian
论文数: 0引用数: 0
h-index: 0
机构:
Chinese Acad Sci, Acad Math & Syst Sci, Inst Appl Math, Beijing 100190, Peoples R ChinaUniv Roma La Sapienza, ICRANet, I-65122 Pescara, Italy
Cao, Zhoujian
[3
]
机构:
[1] Univ Roma La Sapienza, ICRANet, I-65122 Pescara, Italy
[2] Univ Roma La Sapienza, Dept Phys, I-65122 Pescara, Italy
[3] Chinese Acad Sci, Acad Math & Syst Sci, Inst Appl Math, Beijing 100190, Peoples R China
A new scheme for computing dynamical evolutions and gravitational radiations for intermediate-mass-ratio inspirals (IMRIs) based on an effective one-body (EOB) dynamics plus Teukolsky perturbation theory is built in this paper. In the EOB framework, the dynamic essentially affects the resulted gravitational waveform for a binary compact star system. This dynamic includes two parts. One is the conservative part, which comes from effective one-body reduction. The other part is the gravitational backreaction, which contributes to the shrinking process of the inspiral of a binary compact star system. Previous works used an analytical waveform to construct this backreaction term. Since the analytical form is based on post-Newtonian expansion, the consistency of this term is always checked by numerical energy flux. Here, we directly use numerical energy flux by solving the Teukolsky equation via the frequency-domain method to construct this backreaction term. The conservative correction to the leading order terms in mass-ratio is included in the deformed-Kerr metric and the EOB Hamiltonian. We try to use this method to simulate not only quasicircular adiabatic inspiral, but also the nonadiabatic plunge phase. For several different spinning black holes, we demonstrate and compare the resulted dynamical evolutions and gravitational waveforms.