From AAS NOVA: ” A Jet from Neutron Star Merger GW170817″



14 December 2018
Kerry Hensley

This artist’s impression of a black hole that formed after two neutron stars collided shows an accretion disk and a narrow jet. [NASA/CXC/M.Weiss]

Just last year, the three observatories of the Laser Interferometer Gravitational-Wave Observatory (LIGO)–Virgo Collaboration detected the gravitational-wave signature of two neutron stars colliding. What can we learn from the months of observations made since?

On 17 August, 2017, LIGO detected this “chirp” as two neutron stars spiraled inward and collided. This brief gravitational-wave blip, known as GW170817, has been followed up with months of multiwavelength observations. [LSC/Alex Nitz]

When Worlds Collide

Immediately following the detection of gravitational-wave event GW170817, teams of astronomers around the world rushed to pinpoint and characterize the electromagnetic radiation from the source.

These early observations were hugely important for validating our understanding of what happens when neutron stars collide, but the work didn’t end there; in the months that followed, repeated measurements of the flux across the electromagnetic spectrum have provided us with the tools to probe what happened in the aftermath of the merger.

These late-time observations should allow us to distinguish between two competing post-merger scenarios, in which the resultant relativistic jet either pushes past the previously ejected material surrounding the remnant (the “jet-dominated outflow” model) or fails to escape the slow-moving shroud of material (the “cocoon-dominated outflow” model) and is choked.

Radio spectral indices from 6 to 10 months post merger. Combining all the radio data gives a spectral index of -0.53. The black line shown for reference is the radio-to-X-ray spectral index measurement. [Mooley et al. 2018]

Tuning in to GW170817

In order to characterize the nature of the outflow and determine which scenario describes GW170817, a team led by Kunal Mooley (National Radio Astronomy Observatory/Caltech) analyzed the decline of GW170817’s radio emission over time. The authors combined data from multiple radio sources — MeerKAT, Very Large Array (VLA), Giant Metrewave Radio Telescope (uGMRT), and the Australia Telescope Compact Array (ATCA) — to cover the radio emission from 0.65 to 12 GHz.

SKA Meerkat telescope, 90 km outside the small Northern Cape town of Carnarvon, SA

NRAO/Karl V Jansky Expanded Very Large Array, on the Plains of San Agustin fifty miles west of Socorro, NM, USA, at an elevation of 6970 ft (2124 m)

Giant Metrewave Radio Telescope, an array of thirty telecopes, located near Pune in India

CSIRO Australia Compact Array, six radio telescopes at the Paul Wild Observatory, is an array of six 22-m antennas located about twenty five kilometres (16 mi) west of the town of Narrabri in Australia.

After steadily rising for 5–6 months after the event, the radio emission peaked and quickly began to decline, making the transition from rising to falling in just a few weeks. The authors focused on two important features of the radio light curve: how rapidly the flux density decreases after the peak (the power-law decay index) and how “sharp” the peak of the light curve is.

Radio data used in this study. All measurements have been scaled to 3 GHz. The black line is the best-fit model. [Mooley et al. 2018]

Jet vs. Cocoon

Models tell us that if GW170817’s jet were choked by a slow-moving cocoon of material, the radio observations would reveal a power-law decay index of -0.88. If instead the jet punches free of the material as in the jet-dominated outflow model, its flux density would decrease much more rapidly, exhibiting a power-law decay index of -2.17.
So which model do the radio observations of GW170817 support? All of the post-peak data are well-described by a single power-law decay with an index of -2.4. This strongly supports the jet model over the cocoon model, and it suggests that the majority of the energy in the post-merger outflow is carried away by the jet.

The sharpness of the light-curve peak is dependent upon the viewing angle and the width of the jet. Based on a simple jet model, the authors find that the jet is likely very narrow (with an opening angle of less than 10°) and the viewing angle is less than 28°. Future modeling will explore the effects that structure in the jet can have on how sharply peaked the radio light curve is and further our understanding of these highly energetic collisions.


“A Strong Jet Signature in the Late-time Light Curve of GW170817,” K. P. Mooley et al 2018 ApJL 868 L11.

See the full article here .


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