2010ApJ...725.1965L


Query : 2010ApJ...725.1965L

2010ApJ...725.1965L - Astrophys. J., 725, 1965-1970 (2010/December-3)

A new classification method for gamma-ray bursts.

LU H.-J., LIANG E.-W., ZHANG B.-B. and ZHANG B.

Abstract (from CDS):

Recent Swift observations suggest that the traditional long versus short gamma-ray burst (GRB) classification scheme does not always associate GRBs to the two physically motivated model types, i.e., Type II (massive star origin) versus Type I (compact star origin). We propose a new phenomenological classification method of GRBs by introducing a new parameter ε = E γ,iso,52/E 5/3p,z,2, where Eγ,iso is the isotropic gamma-ray energy (in units of 1052 erg) and Ep,z is the cosmic rest-frame spectral peak energy (in units of 100 keV). For those short GRBs with "extended emission," both quantities are defined for the short/hard spike only. With the current complete sample of GRBs with redshift and Epmeasurements, the ε parameter shows a clear bimodal distribution with a separation at ε ∼ 0.03. The high-ε region encloses the typical long GRBs with high luminosity, some high-z "rest-frame-short" GRBs (such as GRB 090423 and GRB 080913), as well as some high-z short GRBs (such as GRB 090426). All these GRBs have been claimed to be of Type II origin based on other observational properties in the literature. All the GRBs that are argued to be of Type I origin are found to be clustered in the low-ε region. They can be separated from some nearby low-luminosity long GRBs (in 3σ) by an additional T90criterion, i.e., T90,z ≲ 5 s in the Swift/BAT band. We suggest that this new classification scheme can better match the physically motivated Type II/I classification scheme.

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

Simbad objects: 36

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Number of rows : 36
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 PSO J027.8085-18.5940 G 01 51 14.05011120 -18 35 38.4976680           ~ 192 0
2 GRB 050406 gB 02 17 52.200 -50 11 15.81     18.83     ~ 125 0
3 PSO J047.1631+13.1580 G 03 08 39.14930640 +13 09 29.0253240           ~ 144 0
4 SN 2006aj SN* 03 21 39.670 +16 52 02.27 17.96 19.11 17.40     SNIc-BL 1007 1
5 GRB 070714B G 03 51 22.2720 +28 17 50.943           ~ 248 0
6 GRB 071227A G 03 52 31.0260 -55 59 00.890           ~ 201 0
7 GRB 080913 gB 04 22 57.90 -25 07 38.6           ~ 213 0
8 GRB 050826 gB 05 51 01.590 -02 38 35.40           ~ 136 0
9 GRB 061006 G 07 24 07.8080 -79 11 55.188           ~ 214 0
10 GRB 071020 gB 07 58 39.65 +32 51 38.8           ~ 158 0
11 SN 2003lw SN* 08 02 30.1 -39 51 03       20.23   SNIc: 576 0
12 SN 2008D SN* 09 09 30.625 +33 08 20.16     17.5     SNIb 458 1
13 SDSS J093805.33+153719.0 G 09 38 05.33384 +15 37 19.0406           ~ 146 0
14 Fermi bn090423330 gB 09 55 33.19 +18 08 57.7           ~ 392 0
15 GRB 061217 gB 10 41 39.320 -21 07 22.11           ~ 128 0
16 GRB 050416 gB 12 33 54.600 +21 03 26.69     19.12     ~ 300 1
17 SDSS J123612.87+285858.8 BiC 12 36 12.8803407000 +28 58 58.780075656           ~ 328 1
18 GRB 090426 G 12 36 18.0470 +32 59 09.460           ~ 237 0
19 GRB 060206 gB 13 31 43.420 +35 03 03.60   19.99 17.09     ~ 330 0
20 GRB 060801 G 14 12 01.2620 +16 58 55.970           ~ 172 0
21 GRB 050813 gB 16 07 57.190 +11 14 57.80           ~ 147 0
22 UGCS J162444.39-273226.8 G 16 24 44.38275 -27 32 26.8381     19.70     ~ 469 1
23 GRB 060926 gB 17 35 43.660 +13 02 18.60     19.36     ~ 135 0
24 GRB 060502B gB 18 35 46.060 +52 37 51.45           ~ 153 1
25 GRB 080520 gB 18 40 46.50 -54 59 30.4           ~ 68 0
26 SN 1998bw SN* 19 35 03.17 -52 50 46.1   14.09       SNIc 1928 2
27 GRB 050922C gB 21 09 33.000 -08 45 30.10 15.15 15.86 14.69     ~ 301 0
28 GRB 060614 G 21 23 32.140 -53 01 36.10           ~ 714 0
29 GRB 070429B G 21 52 03.6910 -38 49 42.820           ~ 125 0
30 GRB 051221 G 21 54 48.626 +16 53 27.16 19.49         ~ 377 0
31 GRB 051210 gB 22 00 40.930 -57 36 47.10           ~ 138 0
32 GRB 060505 gB 22 07 03.440 -27 48 51.89           ~ 286 1
33 GRB 061201 gB 22 08 32.060 -74 34 47.90           ~ 205 0
34 Fermi bn090510016 G 22 14 12.6230 -26 34 58.550           ~ 548 0
35 NVSS J230126-385839 rG 23 01 26.7650 -38 58 40.422   22.22 21.22 21   ~ 325 1
36 GRB 070506 gB 23 08 52.390 +10 43 20.30     19.04     ~ 86 0

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