2013ApJ...766...23R


Query : 2013ApJ...766...23R

2013ApJ...766...23R - Astrophys. J., 766, 23 (2013/March-3)

On the significance of the excess number of strong mg II absorbers observed toward gamma-ray bursts.

RAPOPORT S., ONKEN C.A., WYITHE J.S.B., SCHMIDT B.P. and THYGESEN A.O.

Abstract (from CDS):

The number of strong (equivalent width >1 Å) Mg II absorbers observed toward gamma-ray bursts (GRBs) has been found to be statistically larger than the number of strong absorbers toward quasi-stellar objects (QSOs). We formalize this "Mg II problem" and present a detailed explanation of the statistical tools required to assess the significance of the discrepancy. We find that the problem exists at the 4σ level for GRBs with high-resolution spectra. It has been suggested that the discrepancy can be resolved by the combination of a dust obscuration bias toward QSOs, and a strong gravitational lensing bias toward GRBs. We investigate one of the two most probable lensed GRBs that we presented in our previous work (GRB020405) and find that it is not strongly gravitationally lensed, constraining the percentage of lensed GRBs to be <35% (2σ). Dust obscuration of QSOs has been estimated to be a significant effect with dusty Mg II systems removing ∼20% of absorbed objects from flux-limited QSO samples. We find that if ∼30% of the strong Mg II systems toward QSOs are missing from the observed samples, then GRBs and QSOs would have comparable numbers of absorbers per unit redshift. Thus, strong gravitational lensing bias is likely to make only a modest contribution to solving the Mg II problem. However, if the dust obscuration bias has been slightly underestimated, the Mg II problem would no longer persist.

Abstract Copyright:

Journal keyword(s): gamma-ray burst: general - gamma-ray burst: individual: GRB020405 - gravitational lensing: strong

Simbad objects: 29

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Number of rows : 29
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 071031 gB 00 25 37.40 -58 03 33.9           ~ 167 0
2 GRB 021004 gB 00 26 54.68 +18 55 41.6           ~ 548 0
3 GRB 050908 gB 01 21 50.750 -12 57 17.20           ~ 173 0
4 GRB 991216 gB 05 09 31.2983 +11 17 07.262           ~ 422 0
5 GRB 050505 gB 09 27 03.300 +30 16 23.70     20.74     ~ 192 0
6 GRB 030323 gB 11 06 09.4 -21 46 13           ~ 135 1
7 GRB 011211 gB 11 15 16 -21 56.0           ~ 300 0
8 GRB 030226 gB 11 33 04.9 +25 53 56           ~ 205 0
9 GRB 030328 gB 12 10 48.4 -09 20 51           ~ 144 0
10 GRB 030429 gB 12 13 07.495 -20 54 49.54     23.70     ~ 131 0
11 GRB 060206 gB 13 31 43.420 +35 03 03.60   19.99 17.09     ~ 315 0
12 GRB 020405 gB 13 58 03.12 -31 22 22.2   21.9 21.5     ~ 250 1
13 GRB 050730 gB 14 08 17.090 -03 46 18.90   20.32 17.68     ~ 314 0
14 GRB 080319B gB 14 31 41.04 +36 18 09.2           ~ 469 0
15 GRB 080310 gB 14 40 13.89 -00 10 30.4           ~ 190 0
16 GRB 010222 G 14 52 12.5 +43 01 06           ~ 356 1
17 GRB 060526 gB 15 31 18.360 +00 17 04.90   18.31 17.16     ~ 270 0
18 GRB 060418 gB 15 45 42.600 -03 38 20.00 15.73 16.19 14.98     ~ 361 0
19 GRB 000926 gB 17 04 15 +51 46.0           ~ 366 0
20 Fermi bn081008832 gB 18 39 52.40 -57 25 58.8           ~ 199 0
21 GRB 080413A gB 19 09 11.73 -27 40 39.6           ~ 143 0
22 GRB 020813A gB 19 46 41.874 -19 36 04.81           ~ 304 0
23 GRB 071003 gB 20 07 24.50 +10 56 48.8           ~ 170 0
24 GRB 050922C gB 21 09 33.000 -08 45 30.10 15.15 15.86 14.69     ~ 284 0
25 Fermi bn080804972 gB 21 54 41.90 -53 11 20.2           ~ 138 0
26 GRB 060607 gB 21 58 50.400 -22 29 46.70 18.49 16.67 15.09     ~ 296 0
27 GRB 050820A gB 22 29 38.110 +19 33 37.10 18.33 19.00 18.47     ~ 387 0
28 GRB 081029 gB 23 07 06 -68 10.7           ~ 107 0
29 GRB 051111A gB 23 12 33.170 +18 22 28.80 19.77 20.08 19.50     ~ 207 0

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