Abstract
The merging of a binary system involving two neutron stars (NSs), or a black hole (BH) and a NS, often results in the emission of an electromagnetic (EM) transient. One component of this EM transient is the epic explosion known as a kilonova (KN). The characteristics of the KN emission can be used to probe the equation of state (EoS) of NS matter responsible for its formation. We predict KN light curves from computationally simulated BH-NS mergers, by using the 3D radiative transfer code POSSIS. We investigate two EoSs spanning most of the allowed range of the mass-radius diagram. We also consider a soft EoS compatible with the observational data within the so-called 2-families scenario in which hadronic stars coexist with strange stars. Computed results show that the 2-families scenario, characterized by a soft EoS, should not produce a KN unless the mass of the binary components are small (MBH ≤ 6M⊙, MNS ≤ 1.4M⊙) and the BH is rapidly spinning (χBH ≥ 0.3). In contrast, a strong KN signal potentially observable from future surveys (e.g. VRO/LSST) is produced in the 1-family scenario for a wider region of the parameter space, and even for non-rotating BHs (χBH = 0) when MBH = 4M⊙ and MNS = 1.2M⊙. We also provide a fit that allows for the calculation of the unbound mass from the observed KN magnitude, without running timely and costly radiative transfer simulations. Findings presented in this paper will be used to interpret light curves anticipated during the fourth observing run (O4), of the advanced LIGO, advanced Virgo and KAGRA interferometers and thus to constrain the EoS of NS matter.
Original language | English |
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Pages (from-to) | 11053–11065 |
Journal | Monthly Notices of the Royal Astronomical Society |
Volume | 527 |
Issue number | 4 |
Early online date | 20 Dec 2023 |
DOIs | |
Publication status | Published - 29 Feb 2024 |
Externally published | Yes |
Bibliographical note
The simulations performed in this study will be made publicly available at https://github.com/mbulla/kilonova_models.Funding
This work was supported by the European Union’s Horizon 2020 Programme under the AHEAD2020 project (grant agreement no. 871158) and by the National Science Foundation under grant no. PHY-1430152(JINA Center for the Evolution of the Elements). The simulations were performed on resources provided by the Swedish National Infrastructure for Computing (SNIC) at Kebnekaise partially funded by the Swedish Research Council through grant agreement no. 2018–05973.