Bibcode
DOI
Pedersen, H.; Jaunsen, A. O.; Grav, T.; Ostensen, R.; Andersen, M. I.; Wold, M.; Kristen, H.; Broeils, A.; Naeslund, M.; Fransson, C.; Lacy, M.; Castro-Tirado, A. J.; Gorosabel, J.; Rodríguez-Espinosa, J. M.; Perez, A. M.; Wolf, C.; Fockenbrock, R.; Hjorth, J.; Muhli, P.; Hakala, P.; Piro, L.; Feroci, M.; Costa, E.; Nicastro, L.; Palazzi, E.; Frontera, F.; Monaldi, L.; Heise, J.
Referencia bibliográfica
Astrophysical Journal v.496, p.311
Fecha de publicación:
3
1998
Número de citas
96
Número de citas referidas
83
Descripción
Optical Transients from gamma-ray burst sources, in addition to offering
a distance determination, convey important information about the physics
of the emission mechanism, and perhaps also about the underlying energy
source. As the gamma-ray phenomenon is extremely diverse, with
timescales spanning several orders of magnitude, some diversity in
optical counterpart signatures appears plausible. We have studied the
optical transient that accompanied the gamma-ray burst of 1997 May 8,
GRB 970508. Observations conducted at the 2.5 m Nordic Optical Telescope
(NOT) and the 2.2 m telescope at the German-Spanish Calar Alto
observatory (CAHA) cover the time interval starting 3 hr 5 minutes to 96
days after the high-energy event. This brackets all other published
observations, including radio. When analyzed in conjunction with optical
data from other observatories, evidence emerges for a composite light
curve. The first interval, from 3 to 8 hr after the event, was
characterized by a constant or slowly declining brightness. At a later
moment, the brightness started increasing rapidly, and reached a maximum
approximately 40 hr after the GRB. From that moment, the GRB brightness
decayed approximately as a power law of index -1.21. The last
observation, after 96 days, mR = 24.28 +/- 0.10, is brighter than the
extrapolated power law, and hints that a constant component, mR = 25.50
+/- 0.40, is present. The optical transient is unresolved (FWHM 0."83)
at the faintest magnitude level. The brightness of the optical
transient, its duration, and the general shape of the light curve set
this source apart from the single other optical transient known, that of
the 1997 February 28 event.