Gravitational waves from inspiraling black holes in quadratic gravity

We peform a study of gravitational waves emitted by inspiraling black holes in the context of quadratic gravity. By linearizing the field equations around a flat background, we demonstrate that all degrees of freedom satisfy wave-like equations. These degrees of freedom split into three modes: a massive spin-\(2\) mode, a massive spin-\(0\) mode, and the expected massless spin-\(2\) mode. We construct the energy-momentum tensor of gravitational waves and show that, due to the massive spin-\(2\) mode, it presents the Ostrogradski instability. We also show how to deal with this possible pathology and obtain consistent physical interpretations for the system. Using the energy-momentum tensor, we study the influence of each massive mode in the orbital dynamics and compare it with the standard result of General Relativity. Moreover, we present two methods to constrain the parameter \(\alpha\) associated with the massive spin-\(2\) contribution. From the first method, using the combined waveform for the spin-\(2\) modes, we obtain the constraint \( \alpha \lesssim 1.1 \times 10^{21} m^{2}\). In the second method, using the coalescence time, we get the constraint \( \alpha \lesssim 1.1 \times 10^{13} m^{2}\).