Impact of bulk viscosity on the post-merger gravitational-wave signal from merging neutron stars
Michail Chabanov, Luciano Rezzolla

TL;DR
This study investigates how bulk viscosity affects gravitational-wave signals after neutron star mergers, revealing that higher viscosities damp oscillations but can enhance GW emission and alter the spectrum.
Contribution
First simulations using a second-order relativistic hydrodynamics framework to assess bulk viscosity effects on neutron star merger dynamics and gravitational waves.
Findings
Large viscosities damp post-merger oscillations.
High viscosities preserve deformations, increasing GW emission.
Bulk viscosity can increase GW energy radiated by up to 30%.
Abstract
In the violent post-merger of binary neutron-star mergers strong oscillations are present that impact the emitted gravitational-wave (GW) signal. The frequencies, temperatures and densities involved in these oscillations allow for violations of the chemical equilibrium promoted by weak-interactions, thus leading to a nonzero bulk viscosity that can impact dynamics and GW signals. We present the first simulations of binary neutron-star mergers employing the self-consistent and second-order formulation of the equations of relativistic hydrodynamics for dissipative fluids proposed by M\"uller, Israel and Stewart. With the spirit of obtaining a first assessment of the impact of bulk viscosity on the structure and radiative efficiency of the merger remnant we adopt a simplified but realistic approach for the viscosity, which we assume to be determined by direct and modified Urca reactions…
Peer Reviews
No public reviews on file for this paper yet. If you reviewed it on a platform where reviews are public (OpenReview, ICLR, NeurIPS, ICML), you can paste yours below so the community can read it here.
Videos
No videos yet. Explain this paper in a talk, walkthrough, or lecture? Add one.
Taxonomy
TopicsPulsars and Gravitational Waves Research · Gamma-ray bursts and supernovae · High-Energy Particle Collisions Research
