2011ApJ...732...29C


Query : 2011ApJ...732...29C

2011ApJ...732...29C - Astrophys. J., 732, 29 (2011/May-1)

Afterglow observations of Fermi large area telescope gamma-ray bursts and the emerging class of hyper-energetic events.

CENKO S.B., FRAIL D.A., HARRISON F.A., HAISLIP J.B., REICHART D.E., BUTLER N.R., COBB B.E., CUCCHIARA A., BERGER E., BLOOM J.S., CHANDRA P., FOX D.B., PERLEY D.A., PROCHASKA J.X., FILIPPENKO A.V., GLAZEBROOK K., IVARSEN K.M., KASLIWAL M.M., KULKARNI S.R., LACLUYZE A.P., LOPEZ S., MORGAN A.N., PETTINI M. and RANA V.R.

Abstract (from CDS):

We present broadband (radio, optical, and X-ray) light curves and spectra of the afterglows of four long-duration gamma-ray bursts (GRBs; GRBs 090323, 090328, 090902B, and 090926A) detected by the Gamma-Ray Burst Monitor and Large Area Telescope (LAT) instruments on the Fermi satellite. With its wide spectral bandpass, extending to GeV energies, Fermi is sensitive to GRBs with very large isotropic energy releases (1054 erg). Although rare, these events are particularly important for testing GRB central-engine models. When combined with spectroscopic redshifts, our afterglow data for these four events are able to constrain jet collimation angles, the density structure of the circumburst medium, and both the true radiated energy release and the kinetic energy of the outflows. In agreement with our earlier work, we find that the relativistic energy budget of at least one of these events (GRB 090926A) exceeds the canonical value of 1051 erg by an order of magnitude. Such energies pose a severe challenge for models in which the GRB is powered by a magnetar or a neutrino-driven collapsar, but remain compatible with theoretical expectations for magnetohydrodynamical collapsar models (e.g., the Blandford-Znajek mechanism). Our jet opening angles (θ) are similar to those found for pre-Fermi GRBs, but the large initial Lorentz factors (Γ0) inferred from the detection of GeV photons imply θΓ0 ~ 70-90, values which are above those predicted in magnetohydrodynamic models of jet acceleration. Finally, we find that these Fermi-LAT events preferentially occur in a low-density circumburst environment, and we speculate that this might result from the lower mass-loss rates of their lower-metallicity progenitor stars. Future studies of Fermi-LAT afterglows at radio wavelengths with the order-of-magnitude improvement in sensitivity offered by the Extended Very Large Array should definitively establish the relativistic energy budgets of these events.

Abstract Copyright:

Journal keyword(s): cosmology: observations - gamma-ray burst: general - radio continuum: general

Simbad objects: 33

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Number of rows : 33
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 V* T Phe Mi* 00 30 26.2337742744 -46 24 33.379722396   12.46 11.43 12.43   M7e 72 0
2 GRB 050904 gB 00 54 50.794 +14 05 09.42           ~ 470 0
3 GRB 061007 gB 03 05 19.510 -50 30 02.50 14.28 14.40 12.95     ~ 289 1
4 SN 2006aj SN* 03 21 39.670 +16 52 02.27 17.96 19.11 17.40     SNIc-BL 940 1
5 GRB 991216 gB 05 09 31.2983 +11 17 07.262           ~ 421 0
6 ICRF J054236.1+495107 Sy1 05 42 36.13789710 +49 51 07.2337139   18.45 17.80 17.210   ~ 1494 1
7 GRB 090328 gB 06 02 39.69 -41 52 55.1           ~ 171 1
8 GRB 060729 gB 06 21 31.850 -62 22 12.69           ~ 282 0
9 GRB 970508 gB 06 53 49.2 +79 16 19           ~ 868 1
10 GRB 070125 gB 07 51 17.80 +31 09 04.8           ~ 181 0
11 SN 2003lw SN* 08 02 30.1 -39 51 03       20.23   SNIc: 548 0
12 Fermi bn090423330 gB 09 55 33.19 +18 08 57.7           ~ 357 0
13 Feige 34 HS* 10 39 36.7358839104 +43 06 09.212615280 9.613 10.91 11.14 11.319 11.464 sdOp 681 0
14 GRB 000418 gB 12 25 21 +20 05.0           ~ 214 0
15 Fermi bn090323002 gB 12 42 50.28 +17 03 11.9           ~ 220 1
16 3C 286 Sy1 13 31 08.2883506368 +30 30 32.960091564   17.51 17.25     ~ 4342 2
17 GRB 990510 gB 13 38 07.64 -80 29 48.8           ~ 488 1
18 GRB 020405 gB 13 58 03.12 -31 22 22.2   21.9 21.5     ~ 249 1
19 GRB 080319B gB 14 31 41.04 +36 18 09.2           ~ 467 0
20 GRB 010222 G 14 52 12.5 +43 01 06           ~ 355 1
21 GRB 080721A gB 14 57 55.76 -11 43 24.9           ~ 164 0
22 GRB 990123 gB 15 25 29 +44 45.0     8.95     ~ 989 1
23 GRB 060418 gB 15 45 42.600 -03 38 20.00 15.73 16.19 14.98     ~ 360 0
24 GRB 000301C gB 16 20 18.5 +29 26 35           ~ 356 0
25 GRB 991208 gB 16 33 53.51 +46 27 21.5           ~ 260 1
26 GRB 000926 gB 17 04 15 +51 46.0           ~ 364 0
27 Fermi bn090902462 gB 17 39 45.26 +27 19 28.1           ~ 391 0
28 CD-44 12736 PM* 18 36 25.9502475648 -44 18 36.907592904   10.83 10.22     G0 211 0
29 SN 1998bw SN* 19 35 03.17 -52 50 46.1   14.09       SNIc 1825 2
30 GRB 071003 gB 20 07 24.50 +10 56 48.8           ~ 170 0
31 GRB 050820A gB 22 29 38.110 +19 33 37.10 18.33 19.00 18.47     ~ 386 0
32 Fermi bn090926181 gB 23 33 36.18 -66 19 25.9           ~ 303 0
33 GRB 980703 gB 23 59 06.7 +08 35 07           ~ 445 1

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