6533b871fe1ef96bd12d25e4
RESEARCH PRODUCT
Detection of the high z GRB 080913 and its implications on progenitors and energy extraction mechanisms*
Martín A. GuerreroA. J. Castro-tiradoIstván T. HorváthMartin JelínekAlberto RivaSergei GuziyPéter VeresMiguel-ángel AloyJavier GorosabelD. Perez-ramirezD. Perez-ramirezJ. P. OsborneA. De Ugarte PostigoM. BremerR. S. WarwickPetr KubánekPetr KubánekJ. M. WintersGudlaugur JohannessonK. L. Pagesubject
PhysicsRange (particle radiation)Event horizonAstrophysics (astro-ph)Cosmology: observationsFOS: Physical sciencesAstronomy and AstrophysicsAstrophysicsAstrophysicsRedshiftAfterglowphotometric [techniques]techniques: photometricSpace and Planetary ScienceGRB 090423MillimeterGamma-ray burstobservations [Cosmology]stars: gamma-ray bursts: individual: GRB 080913Energy (signal processing)gamma-ray bursts: individual: GRB 080913 [stars]description
We present multiwavelength observations of one of the most distant gamma-ray bursts detected so far, GRB080913. Based on these observations, we consider whether it could be classified as a short-duration GRB and discuss the implications for the progenitor nature and energy extraction mechanisms. Methods. Multiwavelength X-ray, near IR and millimetre observations were made between 20.7 h and ∼16.8 days after the event. Results. Whereas a very faint afterglow was seen at the 3.5m CAHA telescope in the nIR, the X-ray afterglow was clearly detected in both Swift and XMM-Newton observations. An upper limit is reported in the mm range. We have modeled the data assuming a collimated θ0 3◦ blast wave with an energy injection at ∼0.5 days carrying 5 ∼ 1052 erg or approximately 12 times the initial energy of the blast wave. We find that GRB 080913 shares many of the gamma-ray diagnostics with the more recent burst GRB 090423 for being classified as short had they ocurred at low redshift. If the progenitor were a compact binary merger, it is likely composed by a NS and BH. The Blandford-Znajek (BZ) mechanism is the preferred one to extract energy from the central, maximally-rotating BH. Both the magnetic field close to the event horizon (B) and the BHmass (Mbh) are restricted within a relatively narrow range, such that (B/3× 1016 G)(Mbh/7 M ) ∼ 1. Similar constraints on the central BH hold for collapsar-like progenitor systems if the BZ-mechanism works for the system at hand.
year | journal | country | edition | language |
---|---|---|---|---|
2010-02-18 |