The Broadband Counterpart of the Short GRB 200522A at z = 0.5536: A Luminous Kilonova or a Collimated Outflow with a Reverse Shock?
Creators
- Fong, W.1
- Rastinejad, J.1
- Escorial, A. Rouco1
- Schroeder, G.1
- Kilpatrick, C. D.1
- Paterson, K.1
- Dong, Y.1
- Nugent, A. E.1
- Blanchard, P. K.1
- Goyal, A.1
- Terreran, G.1
- Alexander, K. D.1
- Laskar, T.2
- Barnes, J.3
- Metzger, B. D.3
- Berger, E.4
- Eftekhari, T.4
- Strausbaugh, R.5
- Cucchiara, A.5
- Fryer, C.6
- and others
- 1. Center for Interdisciplinary Exploration and Research in Astrophysics (CIERA) and Department of Physics and Astronomy, Northwestern University, Evanston, IL 60208 (United States)
- 2. Department of Physics, University of Bath, Claverton Down, Bath BA2 7AY (United Kingdom)
- 3. Department of Physics and Columbia Astrophysics Laboratory, Columbia University, New York, NY 10027 (United States)
- 4. Center for Astrophysics - Harvard & Smithsonian, 60 Garden Street, Cambridge, MA 02138 (United States)
- 5. University of the Virgin Islands, #2 Brewers Bay Road, Charlotte Amalie, 00802 USVI (United States)
- 6. Center for Theoretical Astrophysics, Los Alamos National Laboratory, Los Alamos, NM 87545 (United States)
Description
We present the discovery of the radio afterglow and near-infrared (NIR) counterpart of the Swift short gamma-ray burst (GRB) GRB 200522A, located at a small projected offset of ≈1 kpc from the center of a young, star-forming host galaxy at z = 0.5536. The radio and X-ray luminosities of the afterglow are consistent with those of on-axis cosmological short GRBs. The NIR counterpart, revealed by our Hubble Space Telescope observations at a rest-frame time of ≈2.3 days, has a luminosity of ≈(1.3–1.7) × 1042 erg s−1. This is substantially lower than on-axis short GRB afterglow detections but is a factor of ≈8–17 more luminous than the kilonova of GW170817 and significantly more luminous than any kilonova candidate for which comparable observations exist. The combination of the counterpart's color (i − y = −0.08 ± 0.21; rest frame) and luminosity cannot be explained by standard radioactive heating alone. We present two scenarios to interpret the broadband behavior of GRB 200522A: a synchrotron forward shock with a luminous kilonova (potentially boosted by magnetar energy deposition), or forward and reverse shocks from a ≈14°, relativistic (Γ0 ≳ 10) jet. Models that include a combination of enhanced radioactive heating rates, low-lanthanide mass fractions, or additional sources of heating from late-time central engine activity may provide viable alternate explanations. If a stable magnetar was indeed produced in GRB 200522A, we predict that late-time radio emission will be detectable starting ≈0.3–6 yr after the burst for a deposited energy of ≈1053 erg. Counterparts of similar luminosity to GRB 200522A associated with gravitational wave events will be detectable with current optical searches to ≈250 Mpc.
Availability note (English)
Available from http://dx.doi.org/10.3847/1538-4357/abc74aAdditional details
Identifiers
Publishing Information
- Journal Title
- Astrophysical Journal
- Journal Volume
- 906
- Journal Issue
- 2
- Journal Page Range
- [26 p.]
- ISSN
- 0004-637X
- CODEN
- ASJOAB
INIS
- Country of Publication
- United Kingdom
- Country of Input or Organization
- International Atomic Energy Agency (IAEA)
- INIS RN
- 53076241
- Subject category
- S79: ASTROPHYSICS, COSMOLOGY AND ASTRONOMY; S73: NUCLEAR PHYSICS AND RADIATION PHYSICS;
- Descriptors DEI
- AFTERGLOW; COSMIC GAMMA BURSTS; ENERGY ABSORPTION; ENERGY LOSSES; ENGINES; GALAXIES; GRAVITATIONAL WAVES; HEATING RATE; JET MODEL; LUMINOSITY; NEUTRON STARS; RADIATION DETECTION; RARE EARTHS; RELATIVISTIC RANGE; SPACE; SYNCHROTRONS; TELESCOPES; X RADIATION
- Descriptors DEC
- ABSORPTION; ACCELERATORS; COSMIC RADIATION; CYCLIC ACCELERATORS; DETECTION; ELECTROMAGNETIC RADIATION; ELEMENTS; ENERGY RANGE; IONIZING RADIATIONS; LOSSES; MATHEMATICAL MODELS; METALS; OPTICAL PROPERTIES; PARTICLE MODELS; PHYSICAL PROPERTIES; PRIMARY COSMIC RADIATION; RADIATIONS; SORPTION; STARS