2013MNRAS.428.3590T


Query : 2013MNRAS.428.3590T

2013MNRAS.428.3590T - Mon. Not. R. Astron. Soc., 428, 3590-3606 (2013/February-1)

GRB 100219A with X-shooter - abundances in a galaxy at z =4.7.

THONE C.C., FYNBO J.P.U., GOLDONI P., DE UGARTE POSTIGO A., CAMPANA S., VERGANI S.D., COVINO S., KRUHLER T., KAPER L., TANVIR N., ZAFAR T., D'ELIA V., GOROSABEL J., GREINER J., GROOT P., HAMMER F., JAKOBSSON P., KLOSE S., LEVAN A.J., MILVANG-JENSEN B., NICUESA GUELBENZU A., PALAZZI E., PIRANOMONTE S., TAGLIAFERRI G., WATSON D., WIERSEMA K. and WIJERS R.A.M.J.

Abstract (from CDS):

Abundances of galaxies at redshifts z > 4 are difficult to obtain from damped Lyα (DLA) systems in the sightlines of quasars (QSOs) due to the Lyα forest blanketing and the low number of high-redshift QSOs known to date. Gamma-ray bursts (GRBs) with their higher luminosity are well suited to study galaxies out to the formation of the first stars at z > 10. The large wavelength coverage of the X-shooter spectrograph makes it an excellent tool to study the interstellar medium of high-redshift galaxies, in particular if the redshift is not known beforehand. In this paper, we determine the properties of a GRB host at z = 4.66723 from absorption lines combined with X-ray and optical imaging data. This is one of the highest redshifts where a detailed analysis with medium-resolution data is possible. We measure a relatively high metallicity of [S/H] = -1.1±0.2 for a galaxy at this redshift. Assuming ultraviolet pumping as origin for the fine-structure lines, the material observed is between 0.3 and 1.0 kpc from the GRB. The extinction determined by the spectral slope from X-rays to the infrared shows a moderate value of AV = 0.13±0.05 mag and relative abundances point to a warm disc extinction pattern. Low- and high-ionization as well as fine-structure lines show a complicated kinematic structure probably pointing to a merger in progress. We also detect one intervening system at z = 2.18. GRB-DLAs have a shallower evolution of metallicity with redshift than QSO absorbers and no evolution in their Hi column density or ionization fraction. GRB hosts at high redshifts seem to continue the trend of the metallicity-luminosity relation towards lower metallicities but the sample is still too small to draw a definite conclusion. While the detection of GRBs at z > 4 with current satellites is still difficult, they are very important for our understanding of the early epochs of star and galaxy formation.

Abstract Copyright: © 2012 The Authors Published by Oxford University Press on behalf of the Royal Astronomical Society (2012)

Journal keyword(s): galaxies: abundances - galaxies: high-redshift - galaxies: ISM - gamma-ray burst: individual: GRB 100219A

CDS comments: Table 4: GRB 090226A is a misprint for GRB 090926A.

Simbad objects: 47

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Number of rows : 47
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 071031 gB 00 25 37.40 -58 03 33.9           ~ 184 0
2 GRB 050904 gB 00 54 50.794 +14 05 09.42           ~ 496 0
3 GRB 070802 gB 02 27 35.91 -55 31 39.1           ~ 168 0
4 GRB 060223A gB 03 40 49.560 -17 07 48.40     17.90     ~ 98 0
5 GRB 060223 gB 03 40 52.0 -17 08 19           ~ 26 0
6 GRB 111008A gB 04 01 48.220 -32 42 34.09           ~ 127 0
7 GRB 080913 gB 04 22 57.90 -25 07 38.6           ~ 213 0
8 GD 71 WD* 05 52 27.6198591816 +15 53 13.228887444 11.675 12.783 13.032 13.169 13.337 DA1.5 407 0
9 GRB 090429A gB 06 02 13.28 -52 23 14.5           ~ 30 0
10 GRB 000131 gB 06 13 31.08 -51 56 41.7     24.7     ~ 172 1
11 GRB 080129 gB 07 01 08.13 -07 50 47.8           ~ 85 0
12 GRB 080916C gB 07 59 23.24 -56 38 16.8           ~ 386 0
13 Fermi bn090516353 gB 09 12 59 -11 50.9           ~ 173 0
14 GRB 050505 gB 09 27 03.300 +30 16 23.70     20.74     ~ 206 0
15 Fermi bn090423330 gB 09 55 33.19 +18 08 57.7           ~ 392 0
16 GRB 100219A gB 10 16 48.48 -12 34 00.0           ~ 130 0
17 GRB 030323 gB 11 06 09.4 -21 46 13           ~ 138 1
18 GRB 011211 gB 11 15 16 -21 56.0           ~ 305 0
19 GRB 100513A gB 11 18 26.83 +03 37 40.8           ~ 74 0
20 GRB 030226 gB 11 33 04.9 +25 53 56           ~ 212 0
21 GRB 090426 G 12 36 18.0470 +32 59 09.460           ~ 237 0
22 GRB 080607A gB 12 59 47.14 +15 55 09.6           ~ 257 0
23 GRB 100302A gB 13 02 03.66 +74 35 22.5           ~ 83 0
24 GRB 090313 gB 13 13 36.00 +08 05 10.7           ~ 149 0
25 GRB 060206 gB 13 31 43.420 +35 03 03.60   19.99 17.09     ~ 330 0
26 GRB 080825B gB 13 56 48.2 -68 57 18           ~ 17 0
27 GRB 090429B gB 14 02 40.10 +32 10 14.6           ~ 166 0
28 GRB 050730 gB 14 08 17.090 -03 46 18.90   20.32 17.68     ~ 327 0
29 GRB 080310 gB 14 40 13.89 -00 10 30.4           ~ 214 0
30 GRB 090205 gB 14 43 40.00 -27 50 51.4           ~ 99 0
31 GRB 060526 gB 15 31 18.360 +00 17 04.90   18.31 17.16     ~ 288 0
32 GRB 060510B gB 15 56 29.200 +78 34 12.00           ~ 155 0
33 GRB 050401 gB 16 31 28.84 +02 11 14.5           ~ 348 0
34 GRB 080210 gB 16 45 04.03 +13 49 36.3           ~ 121 0
35 GRB 000926 gB 17 04 15 +51 46.0           ~ 373 0
36 GRB 050814 gB 17 36 45.390 +46 20 21.60           ~ 166 0
37 Fermi bn081008832 gB 18 39 52.40 -57 25 58.8           ~ 224 0
38 GRB 080413A gB 19 09 11.73 -27 40 39.6           ~ 163 0
39 GRB 100425A gB 19 56 47.16 -26 25 50.5           ~ 91 0
40 GRB 050922C gB 21 09 33.000 -08 45 30.10 15.15 15.86 14.69     ~ 301 0
41 GRB 060522 gB 21 31 44.850 +02 53 10.80           ~ 140 0
42 GRB 090809 gB 21 54 43.2 -00 05 02           ~ 90 0
43 GRB 060927A gB 21 58 11.930 +05 21 50.32           ~ 215 0
44 GRB 050820A gB 22 29 38.110 +19 33 37.10 18.33 19.00 18.47     ~ 409 0
45 Fermi bn090926181 gB 23 33 36.18 -66 19 25.9           ~ 339 0
46 GRB 071025 gB 23 40 17.02 +31 46 42.4           ~ 122 0
47 NAME Local Group GrG ~ ~           ~ 9325 0

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