# Observable Features of GW170817 Kilonova Afterglow

## TL;DR

This paper models the non-thermal afterglow from GW170817's kilonova ejecta, showing how radio and X-ray observations over years can reveal details about the ejecta's velocity distribution and energy.

## Contribution

It introduces a power-law model for ejecta velocity distribution and predicts observable afterglow signatures that can constrain merger dynamics.

## Key findings

- Detectable radio and X-ray afterglow for typical ejecta parameters.
- Afterglow peaks around a decade post-merger.
- Radio centroid shift indicates ejecta rebrightening.

## Abstract

The neutron star merger, GW170817, was followed by an optical-infrared transient (a kilonova) which indicated that a substantial ejection of mass at trans-relativistic velocities occurred during the merger. Modeling of the kilonova is able to constrain the kinetic energy of the ejecta and its characteristic velocity, but not the high-velocity distribution of the ejecta. Yet, this distribution contains crucial information on the merger dynamics. In this work, we assume a power-law distribution of the form $E(>\beta\Gamma)\propto(\beta\Gamma)^{-\alpha}$ for the energy of the kilonova ejecta and calculate the non-thermal signatures produced by the interaction of the ejecta with the ambient gas. We find that ejecta with minimum velocity $\beta_0\simeq 0.3$ and energy $E\sim 10^{51}$ erg, as inferred from kilonova modeling, has a detectable radio, and possibly X-ray, afterglow for a broad range of parameter space. This afterglow component is expected to dominate the observed emission on a timescale of a few years post merger and peak around a decade later. Its light curve can be used to determine properties of the kilonova ejecta and in particular the ejecta velocity distribution $\alpha$, the minimum velocity $\beta_0$ and its total kinetic energy $E$. We also predict that an afterglow rebrightening, that is associated with the kilonova component, will be accompanied by a shift of the centroid of the radio source towards the initial position of the explosion.