Abstract
Abstract
The ever-increasing number of detections of gravitational waves from compact binaries by the Advanced LIGO and Advanced Virgo detectors allows us to perform ever-more sensitive tests of general relativity (GR) in the dynamical and strong-field regime of gravity. We perform a suite of tests of GR using the compact binary signals observed during the second half of the third observing run of those detectors. We restrict our analysis to the 15 confident signals that have false alarm rates ≤10 −3 yr −1 . In addition to signals consistent with binary black hole mergers, the new events include GW200115_042309, a signal consistent with a neutron star–black hole merger. We find the residual power, after subtracting the best fit waveform from the data for each event, to be consistent with the detector noise. Additionally, we find all the post-Newtonian deformation coefficients to be consistent with the predictions from GR, with an improvement by a factor of ∼2 in the −1PN parameter. We also find that the spin-induced quadrupole moments of the binary black hole constituents are consistent with those of Kerr black holes in GR. We find no evidence for dispersion of gravitational waves, non-GR modes of polarization, or post-merger echoes in the events that were analyzed. We update the bound on the mass of the graviton, at 90% credibility, to ≤2.42×10 −23 eV/ 2 . The final mass and final spin as inferred from the premerger and postmerger parts of the waveform are consistent with each other. The studies of the properties of the remnant black holes, including deviations of the quasinormal mode frequencies and damping times, show consistency with the predictions of GR. In addition to considering signals individually, we also combine results from the catalog of gravitational waves signals to calculate more precise population constraints. We find no evidence in support of physics beyond general relativity.
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@article{Alarcn2025Tests,
title = {Tests of general relativity with GWTC-3},
author = {P. F. de Alarcón and S. Albanesi and R. A. Alfaidi and A. Allocca and P. A. Altin and A. Amato and Christopher Kumar Anand and Shreya Anand and A. Ananyeva and S. B. Anderson and W. G. Anderson and Makoto Ando and T. Andrade and N. Andres and M. Andrés‐Carcasona and T. Andrić and S. V. Angelova and Stefano Ansoldi and Javier M. Antelis and S. Antier and Theocharis A. Apostolatos and E. Z. Appavuravther and S. Appert and S. K. Apple and K. Arai and A. Araya and M. C. Araya and J. S. Areeda and M. Arène and N. Aritomi and N. Arnaud and M. Arogeti and K. G. Arun and Hideki Asada and Y. Asali and G. Ashton and Y. Aso and M. Assiduo and S. Assis de Souza Melo and S. M. Aston and P. Astone and F. Aubin and K. AultONeal and C. Austin and S. Babak and F. Badaracco and M. K. M. Bader and C. Badger and S. Bae and Y. Bae and A. M. Baer and S. Bagnasco and J. Baird and R. Bajpai and T. Baka and M. Ball and G. Ballardin and S. Ballmer and A. Balsamo and G. Baltus and S. Banagiri and B. Banerjee and D. Bankar and J. C. Barayoga and C. Barbieri and B. C. Barish and D. Barker and P. Barneo and F. Barone and B. Barr and L. Barsotti and M. Barsuglia and D. Barta and J. Bartlett and M. A. Barton and I. Bartos and S. Basak and R. Bassiri and A. Basti and M. Bawaj and T. Akutsu and R. Abbott and H. Abe and F. Acernese and K. Ackley and N. Adhikari and R. X. Adhikari and V.K Adkins and V. B. Adya and C. Affeldt and D. Agarwal and M. Agathos and K. Agatsuma and N. Aggarwal and Odylio D. Aguiar and L. Aiello and A. Ain and P. Ajith},
journal = {Physical review. D/Physical review. D.},
year = {2025},
doi = {10.1103/physrevd.112.084080},
url = {https://doi.org/10.1103/physrevd.112.084080}
}
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