2012A&A...548A..11D


Query : 2012A&A...548A..11D

2012A&A...548A..11D - Astronomy and Astrophysics, volume 548A11-11 (2012/12-1)

The distribution of equivalent widths in long GRB afterglow spectra.

DE UGARTE POSTIGO A., FYNBO J.P.U., THOENE C.C., CHRISTENSEN L., GOROSABEL J., MILVANG-JENSEN B., SCHULZE S., JAKOBSSON P., WIERSEMA K., SANCHEZ-RAMIREZ R., LELOUDAS G., ZAFAR T., MALESANI D. and HJORTH J.

Abstract (from CDS):

The extreme brightness of gamma-ray burst (GRB) afterglows and their simple spectral shape make them ideal beacons to study the interstellar medium of their host galaxies through absorption line spectroscopy at almost any redshift. We describe the distribution of rest-frame equivalent widths (EWs) of the most prominent absorption features in GRB afterglow spectra, providing the means to compare individual spectra to the sample and identify its peculiarities. Using 69 low-resolution GRB afterglow spectra, we conduct a study of the rest-frame EWs distribution of features with an average rest-frame EW larger than 0.5Å. To compare an individual GRB with the sample, we develop EW diagrams as a graphical tool, and we give a catalogue with diagrams for the 69 spectra. We introduce a line strength parameter (LSP) that allows us to quantify the strength of the absorption features in a GRB spectrum as compared to the sample by a single number. Using the distributions of EWs of single-species features, we derive the distribution of their column densities by a curve of growth (CoG) fit. We find correlations between the LSP and the extinction of the GRB, the UV brightness of the host galaxies and the neutral hydrogen column density. However, we see no significant evolution of the LSP with the redshift. There is a weak correlation between the ionisation of the absorbers and the energy of the GRB, indicating that, either the GRB event is responsible for part of the ionisation, or that galaxies with high-ionisation media produce more energetic GRBs. Spectral features in GRB spectra are, on average, 2.5 times stronger than those seen in QSO intervening damped Lyman-α (DLA) systems and slightly more ionised. In particular we find a larger excess in the EW of CIVλλ1549 relative to QSO DLAs, which could be related to an excess of Wolf-Rayet stars in the environments of GRBs. From the CoG fitting we obtain an average number of components in the absorption features of GRBs of 6.00–1.25+1.00. The most extreme ionisation ratios in our sample are found for GRBs with low neutral hydrogen column density, which could be related to ionisation by the GRB emission.

Abstract Copyright: ∼

Journal keyword(s): gamma-ray burst: general - techniques: spectroscopic - galaxies: ISM - galaxies: high-redshift - dust, extinction

Simbad objects: 74

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Number of rows : 74
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 080710 gB 00 33 05.68 +19 30 05.8           ~ 136 0
5 GRB 050824 gB 00 48 56.100 +22 36 32.00 19.66 21.03 20.46 23.70   ~ 184 0
6 GRB 050908 gB 01 21 50.750 -12 57 17.20           ~ 179 0
7 GRB 060908 gB 02 07 18.360 +00 20 31.20 16.99 18.34 16.85     ~ 217 0
8 GRB 080707 gB 02 10 28.48 +33 06 35.1           ~ 83 0
9 GRB 070721B gB 02 12 32.98 -02 11 39.8           ~ 128 0
10 GRB 070802 gB 02 27 35.91 -55 31 39.1           ~ 168 0
11 GRB 080411 gB 02 31 54.82 -71 18 07.5           ~ 109 0
12 GRB 071112C gB 02 36 50.89 +28 22 16.9           ~ 164 0
13 GRB 060906 gB 02 43 00.900 +30 21 42.12     19.84     ~ 147 0
14 GRB 061007 gB 03 05 19.510 -50 30 02.50 14.28 14.40 12.95     ~ 315 1
15 GRB 070318 gB 03 13 56.830 -42 56 46.30 18.27 16.23 15.49     ~ 170 0
16 GRB 060115 gB 03 36 08.400 +17 20 43.00           ~ 179 0
17 GRB 060210 gB 03 50 57.370 +27 01 34.40   20.27       ~ 275 0
18 GRB 060904B gB 03 52 50.520 -00 43 30.61 18.27 19.14 18.37     ~ 208 0
19 GRB 080913 gB 04 22 57.90 -25 07 38.6           ~ 213 0
20 GRB 060124 gB 05 08 25.900 +69 44 26.98   18.91 17.35     ~ 280 0
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 070411 gB 07 09 19.930 +01 03 52.60     17.94     ~ 138 0
24 GRB 070125 gB 07 51 17.80 +31 09 04.8           ~ 188 0
25 GRB 071020 gB 07 58 39.65 +32 51 38.8           ~ 158 0
26 GRB 090102 gB 08 32 59.50 +33 06 25.7           ~ 253 0
27 Fermi bn090516353 gB 09 12 59 -11 50.9           ~ 173 0
28 Fermi bn090519881 gB 09 29 16.20 +00 11 23.9           ~ 98 0
29 GRB 061021 gB 09 40 36.120 -21 57 05.40 18.21 19.20 16.82     ~ 160 0
30 GRB 061121 gB 09 48 54.570 -13 11 42.68 17.19 17.71 17.02     ~ 350 0
31 GRB 070306 gB 09 52 23.220 +10 28 55.20           ~ 222 1
32 Fermi bn090423330 gB 09 55 33.19 +18 08 57.7           ~ 392 0
33 GRB 050319 gB 10 16 47.900 +43 32 53.80   18.02 17.01     ~ 274 0
34 GRB 080330 gB 11 17 06.70 +30 36 24.1           ~ 145 0
35 GRB 080603B gB 11 46 07.46 +68 03 38.5           ~ 153 0
36 GRB 050408 gB 12 02 17.320 +10 51 10.00           ~ 153 0
37 GRB 070419A gB 12 10 58.830 +39 55 34.06 18.52         ~ 130 0
38 GRB 090426 G 12 36 18.0470 +32 59 09.460           ~ 237 0
39 GRB 080607A gB 12 59 47.14 +15 55 09.6           ~ 257 0
40 GRB 060206 gB 13 31 43.420 +35 03 03.60   19.99 17.09     ~ 330 0
41 GRB 090429B gB 14 02 40.10 +32 10 14.6           ~ 166 0
42 GRB 050730 gB 14 08 17.090 -03 46 18.90   20.32 17.68     ~ 327 0
43 GRB 090529 gB 14 09 52.49 +24 27 33.5           ~ 89 0
44 GRB 080319B gB 14 31 41.04 +36 18 09.2           ~ 508 0
45 GRB 050802 gB 14 37 05.820 +27 47 12.62 16.85 17.38 16.97     ~ 186 0
46 GRB 080721A gB 14 57 55.76 -11 43 24.9           ~ 180 0
47 GRB 060714 gB 15 11 26.450 -06 33 58.30   20.21 18.54     ~ 209 0
48 GRB 060526 gB 15 31 18.360 +00 17 04.90   18.31 17.16     ~ 288 0
49 GRB 080604 gB 15 47 51.64 +20 33 28.5           ~ 71 0
50 GRB 090814 gB 15 58 26.350 +25 37 52.42           ~ 12 0
51 GRB 090814A gB 15 58 26.44 +25 37 52.4           ~ 56 0
52 GRB 060502A gB 16 03 42.480 +66 36 02.49     18.65     ~ 143 0
53 GRB 050401 gB 16 31 28.84 +02 11 14.5           ~ 348 0
54 GRB 080210 gB 16 45 04.03 +13 49 36.3           ~ 121 0
55 GRB 080319C gB 17 15 55.48 +55 23 31.7           ~ 174 0
56 GRB 080605 gB 17 28 30.04 +04 00 56.9           ~ 198 0
57 GRB 060926 gB 17 35 43.660 +13 02 18.60     19.36     ~ 135 0
58 Fermi bn081008832 gB 18 39 52.40 -57 25 58.8           ~ 224 0
59 GRB 080520 gB 18 40 46.50 -54 59 30.4           ~ 68 0
60 SN 1998bw SN* 19 35 03.17 -52 50 46.1   14.09       SNIc 1928 2
61 Fermi bn080905705 gB 20 06 57.93 -62 33 46.8           ~ 119 0
62 GRB 070508 gB 20 51 11.810 -78 23 04.88     19.62     ~ 144 0
63 GRB 050922C gB 21 09 33.000 -08 45 30.10 15.15 15.86 14.69     ~ 301 0
64 GRB 060614 G 21 23 32.140 -53 01 36.10           ~ 714 0
65 GRB 061110B gB 21 35 40.400 +06 52 34.10           ~ 91 0
66 GRB 080413B gB 21 44 34.62 -19 58 51.2           ~ 191 0
67 GRB 060927A gB 21 58 11.930 +05 21 50.32           ~ 215 0
68 Fermi bn080916406 gB 22 25 09.30 -57 01 33.7           ~ 177 0
69 GRB 061110A gB 22 25 09.800 -02 15 30.70 21.43         ~ 134 0
70 SN 2008hw SN* 22 39 50.39 -40 08 49.1           SNIc 197 1
71 GRB 070506 gB 23 08 52.390 +10 43 20.30     19.04     ~ 86 0
72 GRB 090812 gB 23 32 48.5 -10 36 17           ~ 165 0
73 Fermi bn080810549 gB 23 47 08.00 +00 18 35.1           ~ 240 0
74 GRB 060707 gB 23 48 19.000 -17 54 17.00     19.79     ~ 170 0

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