2022ApJ...940....5D


Query : 2022ApJ...940....5D

2022ApJ...940....5D - Astrophys. J., 940, 5 (2022/November-3)

Reclassifying Swift Gamma-Ray Bursts with Diverse Duration Distributions.

DENG Q., ZHANG Z.-B., LI X.-J., CHANG H.-Y., ZHANG X.-L., ZHEN H.-Y., SUN H., PAN Q. and DONG X.-F.

Abstract (from CDS):

We select the largest sample of Swift gamma-ray bursts (GRBs) so far to reexamine the classification in terms of time duration, hardness ratio, and physical collapse model. To analyze the sample selection effect, we divide the observed Swift GRB sample into four subsamples according to signal-to-noise level, spectral quality, and extended emission. First, we find that only the sample of Swift GRBs with well-measured peak energy can be evidently divided into two types at a boundary of ∼1 s, and other data sets are well described by three Gaussian functions. Using Swift GRBs with known redshift, a Kolmogorov-Smirnov test shows the intrinsic duration distributions of five data sets are equally distributed. Second, we ascertain in the plane of hardness ratio versus duration that the hardness ratio of short GRBs is significantly higher than those of middle classes and long GRBs, while the latter two components are the same in statistics, implying the so-called middle class to be artificial. Third, we apply a collapse model to discriminate the boundaries between collapse and noncollapse Swift bursts. It is interesting to find that a significant fraction, ≥30%, of Swift short GRBs could have originated from the collapsing progenitors, while all long GRBs are produced from the collapsars only. Finally, we point out that short GRBs with extended emission are the main contributors to the noncollapsar population with longer duration.

Abstract Copyright: © 2022. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Gamma-ray bursts

Simbad objects: 17

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Number of rows : 17
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 SN 2010ma SN* 00 48 55.35 -34 33 59.5           SNIc 190 1
2 GRB 050824 gB 00 48 56.100 +22 36 32.00 19.66 21.03 20.46 23.70   ~ 184 0
3 SN 2009nz SN* 02 26 19.87 -18 57 08.6           ~ 307 1
4 Fermi bn101011707 gB 03 13 10.62 -65 58 55.6           ~ 48 0
5 Fermi bn100704149 gB 08 54 33.92 -24 12 09.7           ~ 103 0
6 GRB 050215B gB 11 37 48.030 +40 47 43.39           ~ 71 0
7 GRB 070923 gB 12 18 29.5 -38 17 38           ~ 38 0
8 GRB 050416 gB 12 33 54.600 +21 03 26.69     19.12     ~ 300 1
9 GrW 170817 GWE 13 09 48.0850 -23 22 53.343           ~ 2683 0
10 GRB 090429B gB 14 02 40.10 +32 10 14.6           ~ 166 0
11 GRB 080319B gB 14 31 41.04 +36 18 09.2           ~ 508 0
12 GRB 060428B gB 15 41 25.570 +62 01 28.93 20.64 20.62 19.50     ~ 71 0
13 GRB 100418A gB 17 05 26.96 +11 27 41.9           ~ 198 0
14 SN 2005nc SN* 18 32 32.560 +26 20 22.34           SNIc: 400 1
15 GRB 090618 gB 19 36 01.80 +78 21 07.1           ~ 358 0
16 GRB 060614 G 21 23 32.140 -53 01 36.10           ~ 714 0
17 GRB 051109B gB 23 01 50.330 +38 40 46.51           ~ 93 0

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