2018ApJ...863...50S


Query : 2018ApJ...863...50S

2018ApJ...863...50S - Astrophys. J., 863, 50-50 (2018/August-2)

The three-parameter correlations about the optical plateaus of gamma-ray bursts.

SI S.-K., QI Y.-Q., XUE F.-X., LIU Y.-J., WU X., YI S.-X., TANG Q.-W., ZOU Y.-C., WANG F.-F. and WANG X.-G.

Abstract (from CDS):

Well-sampled optical light curves of 50 gamma-ray bursts (GRBs) with plateau features are compiled from the literature. By empirical fitting, we obtained the parameters of the optical plateaus, such as the decay slopes (α1 and α2), the break times (Tb), and the corresponding optical fluxes (Fb) at the break times. The break time of optical plateaus ranges from tens of seconds to 106 s, with a typical value of about 104 s. We have calculated the break luminosity, and it mainly ranges from 1044 erg s–1 to 1047 erg s–1, which is generally two or three orders of magnitude less than the corresponding break luminosity of the X-ray afterglow plateaus. We reanalyzed the optical plateaus and also found that a significantly tighter correlation exists when we added the isotropic equivalent energy of GRBs Eγ,iso into the Lb,z-Tb,z relation. The best-fit correlation is obtained to be Lb,z∝Tb,z–0.9E_γ,iso_0.4. We next explored the possible correlations among Lb,z, Tb,z and Ep,i, and found there is also a tight correlation between them, which takes the form of Lb,z∝Tb,z–0.9Ep,i0.5. We argue that these two tight Lb,z-Tb,z-Eγ,iso and Lb,z-Tb,z-Ep,i correlations are more physical, and it may be directly related to the radiation physics of GRBs. The tight correlations can possibly be used as standard candles.

Abstract Copyright: © 2018. The American Astronomical Society. All rights reserved.

Journal keyword(s): gamma-ray burst: general - radiation mechanisms: non-thermal

Simbad objects: 50

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Number of rows : 50
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 GRB 101225A gB 00 00 47.48 +44 36 01.0           ~ 142 0
2 GRB 070110 gB 00 03 39.270 -52 58 27.00 21.8 21.9 21.2     ~ 202 0
3 GRB 021004 gB 00 26 54.68 +18 55 41.6           ~ 548 0
4 GRB 060708 gB 00 31 13.850 -33 45 32.40 19.07 19.79 17.37     ~ 99 0
5 Fermi bn120729456 gB 00 52 17.84 +49 56 23.1           ~ 99 0
6 GRB 041006 gB 00 54 50.17 +01 14 07.0           ~ 197 2
7 GRB 040924 gB 02 06 22.52 +16 08 48.8           ~ 164 1
8 SN 2009nz SN* 02 26 19.87 -18 57 08.6           ~ 277 1
9 Fermi bn100728439 gB 02 56 13.44 +00 16 51.6           ~ 124 0
10 GRB 060210 gB 03 50 57.370 +27 01 34.40   20.27       ~ 254 0
11 GRB 091029 gB 04 00 40.00 -55 57 12.7           ~ 149 0
12 GRB 061126 gB 05 46 24.460 +64 12 38.49 18.62 18.79 19.20     ~ 173 1
13 GRB 060729 gB 06 21 31.850 -62 22 12.69           ~ 283 0
14 GRB 070411 gB 07 09 19.930 +01 03 52.60     17.94     ~ 128 0
15 Fermi bn120119170 gB 08 00 06.940 -09 04 53.83           ~ 162 0
16 GRB 061021 gB 09 40 36.120 -21 57 05.40 18.21 19.20 16.82     ~ 146 0
17 GRB 050319 gB 10 16 47.900 +43 32 53.80   18.02 17.01     ~ 260 0
18 GRB 100219A gB 10 16 48.48 -12 34 00.0           ~ 113 0
19 SN 2003dh SN* 10 44 50.030 +21 31 18.15     16.2     SNIcpec 1210 1
20 GRB 170519A gB 10 53 42.49 +25 22 26.7           ~ 44 0
21 GRB 080330 gB 11 17 06.70 +30 36 24.1           ~ 134 0
22 GRB 050408 gB 12 02 17.320 +10 51 10.00           ~ 151 0
23 GRB 030328 gB 12 10 48.4 -09 20 51           ~ 144 0
24 GRB 030429 gB 12 13 07.495 -20 54 49.54     23.70     ~ 131 0
25 GRB 050416 gB 12 33 54.600 +21 03 26.69     19.12     ~ 285 1
26 GRB 090426 gB 12 36 19.49 +32 59 05.5           ~ 207 0
27 GRB 070208 gB 13 11 32.607 +61 57 54.37 20.79 20.79 19.86     ~ 108 0
28 GRB 050801 gB 13 36 35.000 -21 55 41.00 15.03 15.82 15.46     ~ 156 0
29 GRB 050730 gB 14 08 17.090 -03 46 18.90   20.32 17.68     ~ 314 0
30 GRB 080310 gB 14 40 13.89 -00 10 30.4           ~ 190 0
31 GRB 010222 G 14 52 12.5 +43 01 06           ~ 356 1
32 GRB 060714 gB 15 11 26.450 -06 33 58.30   20.21 18.54     ~ 193 0
33 GRB 060526 gB 15 31 18.360 +00 17 04.90   18.31 17.16     ~ 270 0
34 GRB 000301C gB 16 20 18.5 +29 26 35           ~ 356 0
35 GRB 050401 gB 16 31 28.84 +02 11 14.5           ~ 337 0
36 GRB 070518 gB 16 56 47.750 +55 17 41.40 18.68 19.22 19.01     ~ 70 0
37 GRB 100418A gB 17 05 26.96 +11 27 41.9           ~ 182 0
38 GRB 120815A gB 18 15 54.40 -52 07 29.0           ~ 87 0
39 GRB 080413A gB 19 09 11.73 -27 40 39.6           ~ 143 0
40 GRB 090618 gB 19 36 01.80 +78 21 07.1           ~ 323 0
41 GRB 020813A gB 19 46 41.874 -19 36 04.81           ~ 304 0
42 GRB 071003 gB 20 07 24.50 +10 56 48.8           ~ 170 0
43 GRB 050922C gB 21 09 33.000 -08 45 30.10 15.15 15.86 14.69     ~ 284 0
44 GRB 060614 gB 21 23 32.140 -53 01 36.10 18.89 20.12 19.54     ~ 619 1
45 GRB 080413B gB 21 44 34.62 -19 58 51.2           ~ 169 0
46 GRB 030723 gB 21 49 24.40 -27 42 47.4           ~ 126 0
47 GRB 051109A gB 22 01 15.320 +40 49 23.70   20.09 20.14     ~ 174 0
48 Fermi bn081109293 gB 22 03 11.50 -54 42 40.5           ~ 111 1
49 GRB 081029 gB 23 07 06 -68 10.7           ~ 107 0
50 GRB 051111A gB 23 12 33.170 +18 22 28.80 19.77 20.08 19.50     ~ 207 0

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