Abstract
Detections of gravitational-wave signals from compact binary coalescences have enabled us to study extreme astrophysical phenomena and explore fundamental physics. A crucial requisite for these studies is to have accurate signal models with characteristic morphologies, which have been challenging for many decades, and researchers are still endeavoring to incorporate important physics. Therefore, morphology-independent methods have been developed for identifying a signal and its reconstruction. The reconstructed signal allows us to test the agreement between the observed signal and the waveform posterior samples from parameter estimation. These methods model observed signals using a nearly orthogonal wavelet basis in the frame of continuous wavelet transformation. Here, we propose log-uniform scales to construct the wavelets, which are are highly redundant (nonorthogonal) compared to the conventional octave scales but more efficient for reconstructing the signals at high frequencies. And we introduce a semi-model-dependent reconstruction method using the posterior samples of the events, where we model the signal using Gabor-Morlet wavelets with log-uniform scales. We demonstrate the ability to detect deviation using a numerical simulation of an eccentric binary black hole merger, where the signal in the data does not belong to the search template waveform manifold. Finally, we apply this method to each binary black hole merger event in GWTC-1. We have found that the signal produced by the GW150914 event has 96% agreement with the waveform posterior samples. As the detector sensitivity improves and the detected population of black hole mergers grows, we expect the proposed method will provide even stronger tests.
| Original language | English |
|---|---|
| Article number | 033078 |
| Pages (from-to) | 1-12 |
| Journal | Physical Review Research |
| Volume | 4 |
| Issue number | 3 |
| DOIs | |
| Publication status | Published - 26 Jul 2022 |
Bibliographical note
Funding Information:I gratefully acknowledge Ayatri Singha, Sudarshan Ghonge, M.K. Haris, Amit Reza, Khun Sang Phukon, Chinmay Kalaghatgi, Bhooshan Gadre, Melissa Lopez Portilla, and Chris Van Den Broeck for helpful comments and suggestions. S.R. was supported by the research program of the Netherlands Organization for Scientific Research (NWO). The material of this paper is based upon work supported by NSF's LIGO Laboratory, which is a major facility fully funded by the National Science Foundation (NSF). I gratefully acknowledge computational resources provided by the LIGO Laboratory and supported by the NSF Grants No. PHY-0757058 and No. PHY-0823459. This research has made use of data, software and/or web tools obtained from the Gravitational Wave Open Science Center, a service of LIGO Laboratory , the LIGO Scientific Collaboration, and the Virgo Collaboration. LIGO is funded by the U.S. National Science Foundation. Virgo is funded by the French Centre National de Recherche Scientifique (CNRS), the Italian Istituto Nazionale di Fisica Nucleare (INFN), and the Dutch Nikhef, with contributions by Polish and Hungarian institutes.
Publisher Copyright:
© 2022 authors. Published by the American Physical Society.
Funding
I gratefully acknowledge Ayatri Singha, Sudarshan Ghonge, M.K. Haris, Amit Reza, Khun Sang Phukon, Chinmay Kalaghatgi, Bhooshan Gadre, Melissa Lopez Portilla, and Chris Van Den Broeck for helpful comments and suggestions. S.R. was supported by the research program of the Netherlands Organization for Scientific Research (NWO). The material of this paper is based upon work supported by NSF's LIGO Laboratory, which is a major facility fully funded by the National Science Foundation (NSF). I gratefully acknowledge computational resources provided by the LIGO Laboratory and supported by the NSF Grants No. PHY-0757058 and No. PHY-0823459. This research has made use of data, software and/or web tools obtained from the Gravitational Wave Open Science Center, a service of LIGO Laboratory , the LIGO Scientific Collaboration, and the Virgo Collaboration. LIGO is funded by the U.S. National Science Foundation. Virgo is funded by the French Centre National de Recherche Scientifique (CNRS), the Italian Istituto Nazionale di Fisica Nucleare (INFN), and the Dutch Nikhef, with contributions by Polish and Hungarian institutes.
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