Version 2 2022-03-28, 14:51Version 2 2022-03-28, 14:51
Version 1 2021-02-01, 15:57Version 1 2021-02-01, 15:57
journal contribution
posted on 2022-03-28, 14:51authored byAlicia Rouco Escorial, Wen-fai Fong, Peter Veres, Tanmoy Laskar, Amy Lien, Kerry Paterson, Maura Lally, Peter K Blanchard, Anya E Nugent, Nial R Tanvir, Dylaan Cornish, Edo Berger, Eric Burns, Brad Cenko, Bethany E Cobb, Antonio Cucchiara, Adam Goldstein, Raffaella Margutti, Brian Metzger, Peter Milne, Andrew Levan, Matt Nicholl, Nathan Smith
We present X-ray and multi-band optical observations of the afterglow and
host galaxy of GRB 180418A, discovered by Swift/BAT and Fermi/GBM. We present a
reanalysis of the GBM and BAT data deriving durations of the prompt emission of
T_90~2.56s and ~1.90s, respectively. Modeling the Fermi/GBM catalog of 1405
bursts (2008-2014) in the Hardness-T_90 plane, we obtain a probability of ~60%
that GRB 180418A is a short-hard burst. From a combination of Swift/XRT and
Chandra observations, the X-ray afterglow is detected to ~38.5 days after the
burst, and exhibits a single power-law decline with F_X proportional to
t^-0.98. Late-time Gemini observations reveal a faint r ~24.95 mag host galaxy
at an angular offset of ~0.16''. At the likely redshift range of z ~1-1.5, we
find that the X-ray afterglow luminosity of GRB 180418A is intermediate between
short and long GRBs at all epochs during which there is contemporaneous data,
and that GRB 180418A lies closer to the E_({\gamma},peak)-E_({\gamma},iso)
correlation for short GRBs. Modeling the multi-wavelength afterglow with the
standard synchrotron model, we derive the burst explosion properties and find a
jet opening angle of {\theta}_j =>9-14 degrees. If GRB 180418A is a short GRB
that originated from a neutron star merger, it has one of the brightest and
longest-lived afterglows along with an extremely faint host galaxy. If instead
the event is a long GRB that originated from a massive star collapse, it has
among the lowest luminosity afterglows, and lies in a peculiar space in terms
of the Hardness-T_90 and E_({\gamma},peak)-E_({\gamma},iso) planes.