2011ApJ...733...97B


Query : 2011ApJ...733...97B

2011ApJ...733...97B - Astrophys. J., 733, 97 (2011/June-1)

First-year results of broadband spectroscopy of the brightest Fermi-GBM gamma-ray bursts.

BISSALDI E., VON KIENLIN A., KOUVELIOTOU C., BRIGGS M.S., CONNAUGHTON V., GREINER J., GRUBER D., LICHTI G., BHAT P.N., BURGESS M., CHAPLIN V., DIEHL R., FISHMAN G.J., FITZPATRICK G., FOLEY S., GIBBY M.H., GILES M.M., GOLDSTEIN A., GUIRIEC S., VAN DER HORST A.J., KIPPEN R.M., LIN L., McBREEN S., MEEGAN C.A., PACIESAS W.S., PREECE R.D., RAU A., TIERNEY D. and WILSON-HODGE C.

Abstract (from CDS):

We present our results of the temporal and spectral analysis of a sample of 52 bright and hard gamma-ray bursts (GRBs) observed with the Fermi Gamma-ray Burst Monitor (GBM) during its first year of operation (2008 July-2009 July).Our sample was selected from a total of 253 GBM GRBs based on the event peak count rate measured between 0.2 and 40 MeV. The final sample comprised of 34 long and 18 short GRBs. These numbers show that the GBM sample contains a much larger fraction of short GRBs than the CGRO/BATSE data set, which we explain as the result of our (different) selection criteria, which favor collection of short, bright GRBs over BATSE. A first by-product of our selection methodology is the determination of a detection threshold from the GBM data alone, above which GRBs most likely will be detected in the MeV/GeV range with the Large Area Telescope on board Fermi. This predictor will be very useful for future multi-wavelength GRB follow-ups with ground- and space-based observatories. Further, we have estimated the burst durations up to 10 MeV and for the first time expanded the duration-energy relationship in the GRB light curves to high energies. We confirm that GRB durations decline with energy as a power law with index approximately -0.4, as was found earlier with the BATSE data and we also notice evidence of a possible cutoff or break at higher energies. Finally, we performed time-integrated spectral analysis of all 52 bursts and compared their spectral parameters with those obtained with the larger data sample of the BATSE data. We find that the two parameter data sets are similar and confirm that short GRBs are in general harder than longer ones.

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Journal keyword(s): gamma-ray burst: general - methods: data analysis

Simbad objects: 53

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Number of rows : 53
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 Fermi bn090227310 gB 00 13.2 -43 00           ~ 26 0
2 Fermi bn090227772 gB 00 47 +32.2           ~ 53 0
3 Fermi bn090308734 gB 01 27.6 -54 18           ~ 21 0
4 Fermi bn081226509 gB 01 42.0 -47 24           ~ 29 0
5 Fermi bn090219074 gB 01 46 +59.2           ~ 15 0
6 Fermi bn081012549 gB 02 00 44 -17 37.6           ~ 43 0
7 GRB 081125 gB 02 51 -18.9           ~ 30 0
8 GRB 081209 gB 03 01 +63.5           ~ 28 0
9 Fermi bn081129161 gB 04 13 -54.9           ~ 21 0
10 GRB 081121 gB 05 57 07.70 -60 36 42.1           ~ 152 0
11 GRB 090328 gB 06 02 39.69 -41 52 55.1           ~ 194 1
12 Fermi bn080925775 gB 06 24.4 +18 12           ~ 28 0
13 Fermi bn080807993 gB 06 47 -16.0           ~ 25 0
14 GRB 090228 gB 07 07.2 -24 18           ~ 45 0
15 GRB 081110 gB 07 27 +21.4           ~ 29 0
16 GRB 081207 gB 07 29.6 +70 30           ~ 26 0
17 GRB 080916C gB 07 59 23.24 -56 38 16.8           ~ 386 0
18 Fermi bn090429753 gB 08 21 +06.2           ~ 22 0
19 GRB 081215A gB 08 22 +54.0           ~ 57 0
20 GRB 090102 gB 08 32 59.50 +33 06 25.7           ~ 253 0
21 Fermi bn081216531 gB 08 37 +07.6           ~ 35 0
22 GRB 090305B gB 09 00.0 +74 18           ~ 22 0
23 Fermi bn081006604 gB 09 28.0 -67 24           ~ 25 0
24 GRB 080817 gB 10 05 09.600 -19 15 36.00           ~ 27 0
25 GRB 090328B gB 10 23 +33.4           ~ 24 0
26 Fermi bn090330279 gB 10 40.8 -08 12           ~ 19 0
27 Fermi bn090626189 gB 11 20 -33.5           ~ 54 0
28 GRB 080723B gB 11 47 19.77 -60 14 27.9           ~ 53 0
29 2B 930131 gB 12 08.2 -08 14           ~ 127 0
30 GRB 080906B gB 12 11.2 -06 24           ~ 25 0
31 GRB 090424 gB 12 38 07.40 +16 49 45.9           ~ 269 0
32 Fermi bn090323002 gB 12 42 50.28 +17 03 11.9           ~ 244 1
33 GRB 100724A gB 12 58 10.38 -11 06 09.3           ~ 198 0
34 Fermi bn090217206 gB 13 40 -08.4           ~ 56 0
35 Fermi bn081101532 gB 13 50 -28.0           ~ 19 0
36 GRB 081224 gB 14 12 35.85 +74 11 59.5           ~ 27 0
37 GRB 081231 gB 14 35 -38.7           ~ 8 0
38 GRB 080825C gB 15 28.8 -04 54           ~ 71 0
39 GRB 090620 gB 15 49.4 +61 09           ~ 29 0
40 Fermi bn081009140 gB 16 42 +18.4           ~ 40 0
41 GRB 090531B gB 16 48 15.0 -36 01 27           ~ 58 0
42 GRB 080802 gB 18 02.9 -32 20           ~ 29 0
43 Fermi bn080905499 G 19 10 42.0450 -18 52 54.510           ~ 200 0
44 Fermi bn080816989 gB 19 18 -06.8           ~ 19 0
45 GRB 090618 gB 19 36 01.80 +78 21 07.1           ~ 358 0
46 4B 941017 gB 20 06.2 +09 49           ~ 93 0
47 Fermi bn090623107 gB 20 36 -43.2           ~ 20 0
48 GRB 090528B gB 20 49 +32.7           ~ 30 0
49 Fermi bn081024891 gB 21 31 36.00 +21 12 14.4           ~ 91 0
50 Fermi bn081126899 gB 21 34 03.54 +48 42 35.2           ~ 76 0
51 Fermi bn090510016 G 22 14 12.6230 -26 34 58.550           ~ 548 0
52 Fermi bn081122520 gB 22 36.4 +40 00           ~ 27 0
53 GRB 090131 gB 23 29.2 +21 12           ~ 37 0

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