2013ApJ...773...82C


Query : 2013ApJ...773...82C

2013ApJ...773...82C - Astrophys. J., 773, 82 (2013/August-3)

An independent measurement of the incidence of Mg II absorbers along gamma-ray burst sight lines: the end of the mystery?

CUCCHIARA A., PROCHASKA J.X., ZHU G., MENARD B., FYNBO J.P.U., FOX D.B., CHEN H.-W., COOKSEY K.L., CENKO S.B., PERLEY D., BLOOM J.S., BERGER E., TANVIR N.R., D'ELIA V., LOPEZ S., CHORNOCK R. and DE JAEGER T.

Abstract (from CDS):

In 2006, Prochter et al. reported a statistically significant enhancement of very strong Mg II absorption systems intervening the sight lines to gamma-ray bursts (GRBs) relative to the incidence of such absorption along quasar sight lines. This counterintuitive result has inspired a diverse set of astrophysical explanations (e.g., dust, gravitational lensing) but none of these has obviously resolved the puzzle. Using the largest set of GRB afterglow spectra available, we reexamine the purported enhancement. In an independent sample of GRB spectra with a survey path three times larger than Prochter et al., we measure the incidence per unit redshift of ≥ 1 Å rest-frame equivalent width Mg II absorbers at z ~ 1 to be ℓ(z) = 0.18±0.06. This is fully consistent with current estimates for the incidence of such absorbers along quasar sight lines. Therefore, we do not confirm the original enhancement and suggest those results suffered from a statistical fluke. Signatures of the original result do remain in our full sample (ℓ(z) shows an ~1.5 enhancement over ℓ(z)QSO), but the statistical significance now lies at ~90% c.l. Restricting our analysis to the subset of high-resolution spectra of GRB afterglows (which overlaps substantially with Prochter et al.), we still reproduce a statistically significant enhancement of Mg II absorption. The reason for this excess, if real, is still unclear since there is no connection between the rapid afterglow follow-up process with echelle (or echellette) spectrographs and the detectability of strong Mg II doublets. Only a larger sample of such high-resolution data will shed some light on this matter.

Abstract Copyright: ∼

Journal keyword(s): gamma-ray burst: general - quasars: absorption lines - techniques: spectroscopic

Simbad objects: 118

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Number of rows : 118
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 070611 gB 00 07 58.000 -29 45 19.40           ~ 94 0
3 GRB 071031 gB 00 25 37.40 -58 03 33.9           ~ 184 0
4 GRB 021004 gB 00 26 54.68 +18 55 41.6           ~ 560 0
5 GRB 060708 gB 00 31 13.850 -33 45 32.40 19.07 19.79 17.37     ~ 109 0
6 GRB 080710 gB 00 33 05.68 +19 30 05.8           ~ 136 0
7 GRB 050908 gB 01 21 50.750 -12 57 17.20           ~ 179 0
8 Fermi bn100814160 gB 01 29 53.61 -17 59 43.6           ~ 219 0
9 GRB 081222 gB 01 30 57.76 -34 05 44.0           ~ 199 0
10 GRB 100901A gB 01 49 03.56 +22 45 30.6           ~ 170 0
11 GRB 100906A gB 01 54 44.19 +55 37 49.8           ~ 233 0
12 Fermi bn091208410 gB 01 57 38.50 +16 52 50.7           ~ 220 0
13 GRB 060908 gB 02 07 18.360 +00 20 31.20 16.99 18.34 16.85     ~ 217 0
14 GRB 110918A gB 02 10 09.39 -27 06 19.6           ~ 83 0
15 GRB 080707 gB 02 10 28.48 +33 06 35.1           ~ 83 0
16 GRB 070721B gB 02 12 32.98 -02 11 39.8           ~ 128 0
17 GRB 070802 gB 02 27 35.91 -55 31 39.1           ~ 168 0
18 GRB 080411 gB 02 31 54.82 -71 18 07.5           ~ 109 0
19 GRB 071112C gB 02 36 50.89 +28 22 16.9           ~ 164 0
20 GRB 060906 gB 02 43 00.900 +30 21 42.12     19.84     ~ 147 0
21 GRB 110213B gB 02 47 01.45 +01 08 46.5           ~ 27 0
22 Fermi bn110213220 gB 02 51 51.37 +49 16 21.2           ~ 175 0
23 GRB 061007 gB 03 05 19.510 -50 30 02.50 14.28 14.40 12.95     ~ 315 1
24 GRB 070318 gB 03 13 56.830 -42 56 46.30 18.27 16.23 15.49     ~ 170 0
25 GRB 060115 gB 03 36 08.400 +17 20 43.00           ~ 179 0
26 GRB 060210 gB 03 50 57.370 +27 01 34.40   20.27       ~ 275 0
27 GRB 060904B gB 03 52 50.520 -00 43 30.61 18.27 19.14 18.37     ~ 208 0
28 GRB 091029 gB 04 00 40.00 -55 57 12.7           ~ 168 0
29 GRB 111008A gB 04 01 48.220 -32 42 34.09           ~ 127 0
30 GRB 080913 gB 04 22 57.90 -25 07 38.6           ~ 213 0
31 GRB 111229A gB 05 05 08.86 -84 42 39.1           ~ 47 0
32 GRB 060124 gB 05 08 25.900 +69 44 26.98   18.91 17.35     ~ 280 0
33 Fermi bn080928628 gB 06 20 16.85 -55 11 59.3           ~ 187 0
34 GRB 060729 gB 06 21 31.850 -62 22 12.69           ~ 303 0
35 GRB 070411 gB 07 09 19.930 +01 03 52.60     17.94     ~ 138 0
36 GRB 070125 gB 07 51 17.80 +31 09 04.8           ~ 188 0
37 GRB 071020 gB 07 58 39.65 +32 51 38.8           ~ 158 0
38 Fermi bn111107035 gB 08 37 54.66 -66 31 12.3           ~ 97 0
39 Fermi bn090516353 gB 09 12 59 -11 50.9           ~ 173 0
40 Fermi bn090519881 gB 09 29 16.20 +00 11 23.9           ~ 98 0
41 GRB 061121 gB 09 48 54.570 -13 11 42.68 17.19 17.71 17.02     ~ 350 0
42 GRB 070306 gB 09 52 23.220 +10 28 55.20           ~ 222 1
43 GRB 071010B gB 10 02 09.20 +45 43 52.2           ~ 173 0
44 GRB 050319 gB 10 16 47.900 +43 32 53.80   18.02 17.01     ~ 274 0
45 GRB 100219A gB 10 16 48.48 -12 34 00.0           ~ 130 0
46 GRB 110205A gB 10 58 31.12 +67 31 31.2           ~ 213 0
47 GRB 030323 gB 11 06 09.4 -21 46 13           ~ 138 1
48 GRB 080330 gB 11 17 06.70 +30 36 24.1           ~ 145 0
49 GRB 100513A gB 11 18 26.83 +03 37 40.8           ~ 74 0
50 GRB 030226 gB 11 33 04.9 +25 53 56           ~ 212 0
51 Fermi bn091020900 gB 11 42 55.20 +50 58 42.0           ~ 188 0
52 GRB 080603B gB 11 46 07.46 +68 03 38.5           ~ 153 0
53 GRB 030429 gB 12 13 07.495 -20 54 49.54     23.70     ~ 132 0
54 GRB 090426 G 12 36 18.0470 +32 59 09.460           ~ 237 0
55 GRB 090424 gB 12 38 07.40 +16 49 45.9           ~ 269 0
56 GRB 070810A gB 12 39 51.18 +10 45 02.8           ~ 80 0
57 Fermi bn090323002 gB 12 42 50.28 +17 03 11.9           ~ 244 1
58 Fermi bn100414097 gB 12 48 30.0 +08 41 35           ~ 136 0
59 GRB 080607A gB 12 59 47.14 +15 55 09.6           ~ 257 0
60 GRB 100302A gB 13 02 03.66 +74 35 22.5           ~ 83 0
61 GRB 060512 gB 13 03 05.810 +41 11 27.21 19.12 19.63 17.20     ~ 142 0
62 GRB 090313 gB 13 13 36.00 +08 05 10.7           ~ 149 0
63 GRB 060206 gB 13 31 43.420 +35 03 03.60   19.99 17.09     ~ 330 0
64 GRB 050801 gB 13 36 35.000 -21 55 41.00 15.03 15.82 15.46     ~ 164 0
65 GRB 050730 gB 14 08 17.090 -03 46 18.90   20.32 17.68     ~ 327 0
66 GRB 090529A gB 14 09 52.56 +24 27 32.2           ~ 23 0
67 GRB 080319B gB 14 31 41.04 +36 18 09.2           ~ 508 0
68 GRB 050802 gB 14 37 05.820 +27 47 12.62 16.85 17.38 16.97     ~ 186 0
69 GRB 080310 gB 14 40 13.89 -00 10 30.4           ~ 214 0
70 GRB 010222 G 14 52 12.5 +43 01 06           ~ 364 1
71 GRB 080721A gB 14 57 55.76 -11 43 24.9           ~ 180 0
72 GRB 060714 gB 15 11 26.450 -06 33 58.30   20.21 18.54     ~ 209 0
73 GRB 060526 gB 15 31 18.360 +00 17 04.90   18.31 17.16     ~ 288 0
74 GRB 060418 gB 15 45 42.600 -03 38 20.00 15.73 16.19 14.98     ~ 389 0
75 GRB 080604 gB 15 47 51.64 +20 33 28.5           ~ 71 0
76 GRB 060510B gB 15 56 29.200 +78 34 12.00           ~ 155 0
77 GRB 060502A gB 16 03 42.480 +66 36 02.49     18.65     ~ 143 0
78 GRB 050401 gB 16 31 28.84 +02 11 14.5           ~ 348 0
79 GRB 080210 gB 16 45 04.03 +13 49 36.3           ~ 121 0
80 GRB 000926 gB 17 04 15 +51 46.0           ~ 373 0
81 GRB 100418A gB 17 05 26.96 +11 27 41.9           ~ 198 0
82 GRB 080319C gB 17 15 55.48 +55 23 31.7           ~ 174 0
83 GRB 080605 gB 17 28 30.04 +04 00 56.9           ~ 198 0
84 GRB 060926 gB 17 35 43.660 +13 02 18.60     19.36     ~ 135 0
85 Fermi bn090902462 gB 17 39 45.26 +27 19 28.1           ~ 440 0
86 GRB 071122 gB 18 26 25.26 +47 04 29.5           ~ 80 0
87 GRB 080603A gB 18 37 37.95 +62 44 39.6           ~ 89 0
88 Fermi bn081008832 gB 18 39 52.40 -57 25 58.8           ~ 224 0
89 GRB 080520 gB 18 40 46.50 -54 59 30.4           ~ 68 0
90 Fermi bn110731465 gB 18 42 00.99 -28 32 13.8           ~ 193 0
91 GRB 070529 gB 18 54 58.230 +20 39 34.00 20.38   17.25     ~ 98 0
92 GRB 110726A gB 19 06 52.21 +56 04 16.4           ~ 55 0
93 GRB 080413A gB 19 09 11.73 -27 40 39.6           ~ 163 0
94 GRB 020813A gB 19 46 41.874 -19 36 04.81           ~ 316 0
95 Fermi bn080905705 gB 20 06 57.93 -62 33 46.8           ~ 119 0
96 GRB 071003 gB 20 07 24.50 +10 56 48.8           ~ 181 0
97 GRB 091109A gB 20 37 00.50 -44 10 36.0           ~ 52 0
98 GRB 080805 gB 20 56 55.30 -62 25 58.8           ~ 102 0
99 GRB 050922C gB 21 09 33.000 -08 45 30.10 15.15 15.86 14.69     ~ 301 0
100 GRB 060522 gB 21 31 44.850 +02 53 10.80           ~ 140 0
101 GRB 061110B gB 21 35 40.400 +06 52 34.10           ~ 91 0
102 GRB 080413B gB 21 44 34.62 -19 58 51.2           ~ 191 0
103 Fermi bn080804972 gB 21 54 41.90 -53 11 20.2           ~ 158 0
104 GRB 060927A gB 21 58 11.930 +05 21 50.32           ~ 215 0
105 GRB 060607 gB 21 58 50.400 -22 29 46.70 18.49 16.67 15.09     ~ 318 0
106 GRB 071117 gB 22 20 10.40 -63 26 36.6           ~ 112 0
107 Fermi bn080916406 gB 22 25 09.30 -57 01 33.7           ~ 177 0
108 GRB 061110A gB 22 25 09.800 -02 15 30.70 21.43         ~ 134 0
109 GRB 050820A gB 22 29 38.110 +19 33 37.10 18.33 19.00 18.47     ~ 409 0
110 Fermi bn091024380 gB 22 37 +56.9           ~ 151 0
111 SN 2008hw SN* 22 39 50.39 -40 08 49.1           SNIc 197 1
112 GRB 081029 gB 23 07 06 -68 10.7           ~ 121 0
113 GRB 070506 gB 23 08 52.390 +10 43 20.30     19.04     ~ 86 0
114 GRB 051111A gB 23 12 33.170 +18 22 28.80 19.77 20.08 19.50     ~ 223 0
115 GRB 090812 gB 23 32 48.5 -10 36 17           ~ 165 0
116 Fermi bn090926181 gB 23 33 36.18 -66 19 25.9           ~ 339 0
117 Fermi bn080810549 gB 23 47 08.00 +00 18 35.1           ~ 240 0
118 GRB 060707 gB 23 48 19.000 -17 54 17.00     19.79     ~ 170 0

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