Modelling kilonova afterglows: Effects of the thermal electron population and interaction with GRB outflows

Author:

Nedora Vsevolod12ORCID,Dietrich Tim12,Shibata Masaru13,Pohl Martin24,Crosato Menegazzi Ludovica1

Affiliation:

1. Max Planck Institute for Gravitational Physics (Albert Einstein Institute) , Am Mühlenberg 1, Potsdam D-14476, Germany

2. Institute for Physics and Astronomy, University of Potsdam , Potsdam D-14476, Germany

3. Center for Gravitational Physics and Quantum Information, Yukawa Institute for Theoretical Physics, Kyoto University , Kyoto, 606-8502, Japan

4. Deutsches Elektronen-Synchrotron DESY , Platanenallee 6, D-15738 Zeuthen, Germany

Abstract

AbstractGiven an increasing number of gamma-ray bursts accompanied by potential kilonovae, there is a growing importance to advance modelling of kilonova afterglows. In this work, we investigate how the presence of two electron populations that follow a Maxwellian (thermal) and a power-law (non-thermal) distribution affect kilonova afterglow light curves. We employ semi-analytic afterglow model, PyBlastAfterglow. We consider kilonova ejecta profiles from ab-initio numerical relativity binary neutron star merger simulations, targeted to GW170817. We do not perform model selection. We find that the emission from thermal electrons dominates at early times. If the interstellar medium density is high (${\simeq }0.1\, \, \text{cm}^{-3}$), it adds an early time peak to the light curve. As ejecta decelerates, the spectral and temporal indexes change in a characteristic way that, if observed, can be used to reconstruct the ejecta velocity distribution. For the low interstellar medium density, inferred for GRB 170817A, the emission from the non-thermal electron population generally dominates. We also assess how kilonova afterglow light curves change if the interstellar medium has been partially removed and pre-accelerated by laterally expanding gamma-ray burst ejecta. For the latter, we consider properties informed by observations of GRB170817A. We find that the main effect is the emission suppression at early time ${\lesssim }10^{3}\,$ days, and at its maximum it reaches ${\sim }40{{\ \rm per\ cent}}$ when the fast tail of the kilonova ejecta moves subsonically through the wake of laterally spreading gamma-ray burst ejecta. The subsequent rebrightening, when these ejecta break through and shocks form, is very mild (${\lesssim }10{{\ \rm per\ cent}}$) and may not be observable.

Funder

GCS

Publisher

Oxford University Press (OUP)

Subject

Space and Planetary Science,Astronomy and Astrophysics

Cited by 4 articles. 订阅此论文施引文献 订阅此论文施引文献,注册后可以免费订阅5篇论文的施引文献,订阅后可以查看论文全部施引文献

1. Neutron-star measurements in the multi-messenger Era;Astroparticle Physics;2024-02

2. Binary neutron star populations in the Milky Way;Monthly Notices of the Royal Astronomical Society;2023-09-14

3. Nucleosynthesis in outflows of compact objects and detection prospects of associated kilonovae;Monthly Notices of the Royal Astronomical Society;2023-08-03

4. Synthetic radio images of structured GRB and kilonova afterglows;Monthly Notices of the Royal Astronomical Society;2023-07-22

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