2015MNRAS.449L...6C


Query : 2015MNRAS.449L...6C

2015MNRAS.449L...6C - Mon. Not. R. Astron. Soc., 449, L6-L10 (2015/May-1)

Selection biases in the gamma-ray burst E_iso - L_opt, X correlation.

COWARD D.M., HOWELL E.J., WAN L. and MacPHERSON D.

Abstract (from CDS):

Gamma-ray burst (GRB) optical and X-ray afterglow luminosity is expected to correlate with the GRB isotropic equivalent kinetic energy of the outflow in the standard synchrotron model for GRB afterglows. Previous studies, using prompt GRB isotropic equivalent energy (Eiso) as a proxy for isotropic equivalent kinetic energy, have generally confirmed a correlation between X-ray and optical afterglow luminosities. Assuming that GRB afterglow luminosity does not evolve strongly with redshift, we identify a strong Malmquist bias in GRB optical and X-ray afterglow luminosity data. We show that selection effects dominate the observed Eiso-Lopt, X correlations, and have likely been underestimated in other studies. The bias is strongest for a subset of optically faint bursts m > 24 at 24 h with z > 2. After removing this optical selection bias, the Eiso-Lopt, X correlation for long GRBs is not statistically significant, but combining both long and short GRB luminosity data the correlation is significant. Using the median of the Eiso and Lopt, X distributions, we apply the synchrotron model assuming the same power-law index for short and long GRBs, but different microphysical parameter distributions. Comparing the ratio of optical and X-ray luminosities, we find tentative evidence that the fraction of post-shock energy in magnetic fields, εB, could be systematically higher in short GRBs compared to long GRBs.

Abstract Copyright: © 2015 The Authors Published by Oxford University Press on behalf of the Royal Astronomical Society (2015)

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

VizieR on-line data: <Available at CDS (J/MNRAS/449/L6): table.dat fig3.dat>

Simbad objects: 77

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Number of rows : 77
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 GRB 070110 gB 00 03 39.270 -52 58 27.00 21.8 21.9 21.2     ~ 220 0
2 GRB 071031 gB 00 25 37.40 -58 03 33.9           ~ 184 0
3 GRB 080710 gB 00 33 05.68 +19 30 05.8           ~ 136 0
4 Fermi bn100117879 G 00 45 04.6610 -01 35 42.020           ~ 155 0
5 GRB 050904 gB 00 54 50.794 +14 05 09.42           ~ 496 0
6 GRB 050908 gB 01 21 50.750 -12 57 17.20           ~ 179 0
7 PSO J027.8085-18.5940 G 01 51 14.05011120 -18 35 38.4976680           ~ 192 0
8 GRB 060908 gB 02 07 18.360 +00 20 31.20 16.99 18.34 16.85     ~ 217 0
9 GRB 070802 gB 02 27 35.91 -55 31 39.1           ~ 168 0
10 GRB 071112C gB 02 36 50.89 +28 22 16.9           ~ 164 0
11 GRB 050603 gB 02 39 56.839 -25 10 54.92     18.48     ~ 174 0
12 GRB 060906 gB 02 43 00.900 +30 21 42.12     19.84     ~ 147 0
13 GRB 061007 gB 03 05 19.510 -50 30 02.50 14.28 14.40 12.95     ~ 315 1
14 GRB 050318 gB 03 18 51.000 -46 23 43.61 18.10 18.68 17.58     ~ 189 0
15 GRB 070714B G 03 51 22.2720 +28 17 50.943           ~ 248 0
16 GRB 071227A G 03 52 31.0260 -55 59 00.890           ~ 201 0
17 GRB 060904B gB 03 52 50.520 -00 43 30.61 18.27 19.14 18.37     ~ 208 0
18 GRB 080913 gB 04 22 57.90 -25 07 38.6           ~ 213 0
19 GRB 060124 gB 05 08 25.900 +69 44 26.98   18.91 17.35     ~ 280 0
20 GRB 061126 gB 05 46 24.460 +64 12 38.49 18.62 18.79 19.20     ~ 182 1
21 Fermi bn080928628 gB 06 20 16.85 -55 11 59.3           ~ 187 0
22 GRB 060729 gB 06 21 31.850 -62 22 12.69           ~ 303 0
23 GRB 080129 gB 07 01 08.13 -07 50 47.8           ~ 85 0
24 GRB 070411 gB 07 09 19.930 +01 03 52.60     17.94     ~ 138 0
25 GRB 061006 G 07 24 07.8080 -79 11 55.188           ~ 214 0
26 GRB 071020 gB 07 58 39.65 +32 51 38.8           ~ 158 0
27 GRB 070612A gB 08 05 28.530 +37 16 09.57           ~ 82 0
28 GRB 090102 gB 08 32 59.50 +33 06 25.7           ~ 253 0
29 SDSS J093805.33+153719.0 G 09 38 05.33384 +15 37 19.0406           ~ 146 0
30 GRB 061121 gB 09 48 54.570 -13 11 42.68 17.19 17.71 17.02     ~ 350 0
31 Fermi bn090423330 gB 09 55 33.19 +18 08 57.7           ~ 392 0
32 GRB 050319 gB 10 16 47.900 +43 32 53.80   18.02 17.01     ~ 274 0
33 GRB 080330 gB 11 17 06.70 +30 36 24.1           ~ 145 0
34 SDSS J112848.22+170418.5 G 11 28 48.22989 +17 04 18.5014           ~ 393 0
35 GRB 070419A gB 12 10 58.830 +39 55 34.06 18.52         ~ 130 0
36 SDSS J123612.87+285858.8 BiC 12 36 12.8803407000 +28 58 58.780075656           ~ 328 1
37 GRB 090426 G 12 36 18.0470 +32 59 09.460           ~ 237 0
38 GRB 090424 gB 12 38 07.40 +16 49 45.9           ~ 269 0
39 GRB 070810A gB 12 39 51.18 +10 45 02.8           ~ 80 0
40 GRB 060512 gB 13 03 05.810 +41 11 27.21 19.12 19.63 17.20     ~ 142 0
41 GRB 070208 gB 13 11 32.607 +61 57 54.37 20.79 20.79 19.86     ~ 119 0
42 GRB 090313 gB 13 13 36.00 +08 05 10.7           ~ 149 0
43 GRB 060206 gB 13 31 43.420 +35 03 03.60   19.99 17.09     ~ 330 0
44 PSO J203.7673-22.1424 G 13 35 04.16044560 -22 08 32.8717680           ~ 178 0
45 GRB 050801 gB 13 36 35.000 -21 55 41.00 15.03 15.82 15.46     ~ 164 0
46 GRB 050730 gB 14 08 17.090 -03 46 18.90   20.32 17.68     ~ 327 0
47 GRB 080319B gB 14 31 41.04 +36 18 09.2           ~ 508 0
48 GRB 080310 gB 14 40 13.89 -00 10 30.4           ~ 214 0
49 GRB 080721A gB 14 57 55.76 -11 43 24.9           ~ 180 0
50 GRB 060714 gB 15 11 26.450 -06 33 58.30   20.21 18.54     ~ 209 0
51 GRB 060526 gB 15 31 18.360 +00 17 04.90   18.31 17.16     ~ 288 0
52 GRB 081203A gB 15 32 07.6 +63 31 15           ~ 177 0
53 GRB 060418 gB 15 45 42.600 -03 38 20.00 15.73 16.19 14.98     ~ 389 0
54 GRB 060502A gB 16 03 42.480 +66 36 02.49     18.65     ~ 143 0
55 GRB 050401 gB 16 31 28.84 +02 11 14.5           ~ 348 0
56 GRB 080210 gB 16 45 04.03 +13 49 36.3           ~ 121 0
57 GRB 071122 gB 18 26 25.26 +47 04 29.5           ~ 80 0
58 SN 2005nc SN* 18 32 32.560 +26 20 22.34           SNIc: 400 1
59 Fermi bn081008832 gB 18 39 52.40 -57 25 58.8           ~ 224 0
60 GRB 080413A gB 19 09 11.73 -27 40 39.6           ~ 163 0
61 Fermi bn080905499 G 19 10 42.0450 -18 52 54.510           ~ 200 0
62 GRB 071010A gB 19 12 14.42 -32 24 06.2           ~ 138 0
63 GRB 071003 gB 20 07 24.50 +10 56 48.8           ~ 181 0
64 GRB 050315 gB 20 25 54.100 -42 36 02.19           ~ 225 0
65 GRB 050922C gB 21 09 33.000 -08 45 30.10 15.15 15.86 14.69     ~ 301 0
66 GRB 060614 G 21 23 32.140 -53 01 36.10           ~ 714 0
67 GRB 060605 gB 21 28 37.320 -06 03 31.30   20.12 16.53     ~ 210 0
68 GRB 051221 G 21 54 48.626 +16 53 27.16 19.49         ~ 377 0
69 GRB 060927A gB 21 58 11.930 +05 21 50.32           ~ 215 0
70 GRB 051109A gB 22 01 15.320 +40 49 23.70   20.09 20.14     ~ 190 0
71 GRB 061201 gB 22 08 32.060 -74 34 47.90           ~ 205 0
72 Fermi bn090510016 G 22 14 12.6230 -26 34 58.550           ~ 548 0
73 GRB 050820A gB 22 29 38.110 +19 33 37.10 18.33 19.00 18.47     ~ 409 0
74 GRB 051111A gB 23 12 33.170 +18 22 28.80 19.77 20.08 19.50     ~ 223 0
75 Fermi bn100816026 gB 23 26 57.56 +26 34 42.6           ~ 170 0
76 Fermi bn080810549 gB 23 47 08.00 +00 18 35.1           ~ 240 0
77 GRB 060707 gB 23 48 19.000 -17 54 17.00     19.79     ~ 170 0

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