2009ApJ...697..345C


Query : 2009ApJ...697..345C

2009ApJ...697..345C - Astrophys. J., 697, 345-360 (2009/May-3)

Testing the possible intrinsic origin of the excess very strong Mg II absorbers along gamma-ray burst lines-of-sight.

CUCCHIARA A., JONES T., CHARLTON J.C., FOX D.B., EINSIG D. and NARAYANAN A.

Abstract (from CDS):

The startling discovery by Prochter et al. that the frequency of very strong (Wr(2796)>1 Å) Mg II absorbers along gamma-ray burst (GRB) lines of sight ([dN/dz]GRB= 0.90) is more than three times the frequency along quasar lines of sight ([dN/dz]QSO= 0.24), over similar redshift ranges, has yet to be understood. In particular, explanations appealing to dust antibias in quasar samples, partial covering of the quasar sources, and gravitational-lensing amplification of the GRBs have all been carefully examined and found wanting. We therefore reconsider the possibility that the excess of very strong Mg II absorbers toward GRBs is intrinsic either to the GRBs themselves or to their immediate environment, and associated with bulk outflows with velocities as large as vmax∼ 0.3c. In order to examine this hypothesis, we accumulate a sample of 27 Wr(2796)>1 Å absorption systems found toward 81 quasars, and compare their properties to those of 8 Wr(2796) > 1 Å absorption systems found toward six GRBs; all systems have been observed at high spectral resolution (R = 45, 000) using the Ultraviolet and Visual Echelle Spectrograph on the Very Large Telescope. We make multiple comparisons of the absorber properties across the two populations, testing for differences in metallicity, ionization state, abundance patterns, dust abundance, kinematics, and phase structure. We find no significant differences between the two absorber populations using any of these metrics, implying that, if the excess of absorbers along GRB lines of sight are indeed intrinsic, they must be produced by a process which has strong similarities to the processes yielding strong Mg II systems associated with intervening galaxies. Although this may seem a priori unlikely, given the high outflow velocities required for any intrinsic model, we note that the same conclusion was reached, recently, with respect to the narrow absorption line systems seen in some quasars.

Abstract Copyright: ∼

Journal keyword(s): gamma rays: bursts - quasars: absorption lines - techniques: spectroscopic

CDS comments: GRB 050111 is a misprint for GRB 051111.

Simbad objects: 32

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Number of rows : 32
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 QSO B0002-422 QSO 00 04 48.2718888096 -41 57 28.148932548   17.44 17.21     ~ 163 0
2 GRB 021004 gB 00 26 54.68 +18 55 41.6           ~ 560 0
3 GRB 050904 gB 00 54 50.794 +14 05 09.42           ~ 496 0
4 PHL 957 QSO 01 03 11.2741573824 +13 16 17.809871484   16.97 16.57     ~ 350 0
5 QSO B0109-353 QSO 01 11 43.6321128912 -35 03 00.587535660   16.6 16.9     ~ 79 0
6 QSO B0112+03 QSO 01 14 53.2286036664 +03 14 56.953353696     18.6     ~ 62 2
7 QSO B0130-403 QSO 01 33 01.9294067496 -40 06 27.997379496   17.68 17.02     ~ 89 0
8 QSO B0237-2322 QSO 02 40 08.1743783856 -23 09 15.729012036   16.78 16.63     ~ 516 1
9 QSO J0330-2704 QSO 03 30 32.5749333264 -27 04 39.242748900     19.00     ~ 23 1
10 QSO J0455-4216 QSO 04 55 23.0626782912 -42 16 17.398553052   17.77 17.06     ~ 144 0
11 QSO B0551-36 QSO 05 52 46.1824785360 -36 37 27.608212524   17.72 17.57     ~ 98 0
12 QSO B0940-1050 QSO 09 42 53.5078384704 -11 04 25.931336376   16.96 16.6 16.6   ~ 102 0
13 NGC 3372 HII 10 45 02.23 -59 41 59.8           ~ 1071 2
14 QSO J1113-1533 QSO 11 13 50.6122921416 -15 33 34.005990672   18.7 18.7     ~ 39 0
15 QSO B1122-168 QSO 11 24 42.8658917592 -17 05 17.389038732   16.5 16.5 16.1   ~ 132 1
16 QSO J1130-1449 Bla 11 30 07.0523452128 -14 49 27.388021944   17.17 16.90 16 16.97 ~ 739 1
17 QSO B1151+068 QSO 11 54 11.0745443880 +06 34 27.165655200     18.6     ~ 59 0
18 4C -02.55 Bla 12 32 00.0159535440 -02 24 04.793069304   17.41 17.06 16.4   ~ 440 1
19 GRB 060206 gB 13 31 43.420 +35 03 03.60   19.99 17.09     ~ 330 0
20 QSO B1331+170 Bla 13 33 35.7827544072 +16 49 04.013500728   16.84 16.71 16.41   ~ 469 1
21 QSO J1344-1035 QSO 13 44 27.0637256688 -10 35 41.741388492     17.1     ~ 54 0
22 GRB 050730 gB 14 08 17.090 -03 46 18.90   20.32 17.68     ~ 327 0
23 QSO B1418-064 Bla 14 21 07.75560722 -06 43 56.3557864   20.4 18.50 19.1   ~ 78 1
24 GRB 060418 gB 15 45 42.600 -03 38 20.00 15.73 16.19 14.98     ~ 389 0
25 QSO B1618-0035 QSO 16 21 16.9228185456 -00 42 50.909201856   18.92 17.97     ~ 86 0
26 4C 23.43 Bla 16 24 39.0838297968 +23 45 12.223370412   17.91 17.47     ~ 343 1
27 4C 12.59 QSO 16 31 45.1708807968 +11 56 03.203387592   18.38 18.40     ~ 122 1
28 GRB 050922C gB 21 09 33.000 -08 45 30.10 15.15 15.86 14.69     ~ 301 0
29 GRB 060607 gB 21 58 50.400 -22 29 46.70 18.49 16.67 15.09     ~ 318 0
30 QSO J2220-2803 QSO 22 20 06.7591541688 -28 03 23.467479516     16.0 16.10   ~ 100 0
31 GRB 050820A gB 22 29 38.110 +19 33 37.10 18.33 19.00 18.47     ~ 409 0
32 GRB 051111A gB 23 12 33.170 +18 22 28.80 19.77 20.08 19.50     ~ 223 0

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