# When Did the Remnant of GW170817 Collapse to a Black Hole?

**Authors:** Ramandeep Gill, Antonios Nathanail, and Luciano Rezzolla

arXiv: 1901.04138 · 2019-05-29

## TL;DR

This paper estimates that the remnant of GW170817 collapsed into a black hole approximately 1 second after the merger, using constraints from ejecta properties and jet breakout timing, informing neutron star merger models.

## Contribution

It introduces a method combining ejecta mass and jet breakout constraints to determine the collapse time of the merger remnant.

## Key findings

- Remnant collapsed to a black hole after about 0.98 seconds.
- The blue ejecta mass and jet breakout timing constrain the collapse time.
- Future observations can further refine the properties of merger remnants.

## Abstract

The main hard pulse of prompt gamma-ray emission in GRB$\,$170817A had a duration of $\sim0.5\,{\rm s}$ and its onset was delayed with respect to the gravitational-wave chirp signal by $t_{\rm del} \approx 1.74\,{\rm s}$. Detailed follow-up of the subsequent broadband kilonova emission revealed a two-component ejecta -- a lanthanide-poor ejecta with mass $M_{\rm ej,blue}\approx0.025\,M_\odot$ that powered the early but rapidly fading blue emission and a lanthanide-rich ejecta with mass $M_{\rm ej,red}\approx 0.04\,M_\odot$ that powered the longer lasting redder emission. Both the prompt gamma-ray onset delay and the existence of the blue ejecta with modest electron fraction, $0.2\lesssim Y_e\lesssim0.3$, can be explained if the collapse to a black hole was delayed by the formation of a hypermassive neutron star (HMNS). Here, we determine the survival time of the merger remnant by combining two different constraints, namely, the time needed to produce the requisite blue-ejecta mass and that necessary for the relativistic jet to bore its way out of the expanding ejecta. In this way, we determine that the remnant of GW170817 must have collapsed to a black hole after $t_{\rm coll}=0.98_{-0.26}^{+0.31}\,{\rm s}$. We also discuss how future detections and the delays between the gravitational and electromagnetic emissions can be used to constrain the properties of the merged object.

## Full text

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## Figures

11 figures with captions in the complete paper: https://tomesphere.com/paper/1901.04138/full.md

## References

171 references — full list in the complete paper: https://tomesphere.com/paper/1901.04138/full.md

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Source: https://tomesphere.com/paper/1901.04138