2019A&A...623A..43B


Query : 2019A&A...623A..43B

2019A&A...623A..43B - Astronomy and Astrophysics, volume 623A, 43-43 (2019/3-1)

Evidence for diffuse molecular gas and dust in the hearts of gamma-ray burst host galaxies. Unveiling the nature of high-redshift damped Lyman-α systems.

BOLMER J., LEDOUX C., WISEMAN P., DE CIA A., SELSING J., SCHADY P., GREINER J., SAVAGLIO S., BURGESS J.M., D'ELIA V., FYNBO J.P.U., GOLDONI P., HARTMANN D.H., HEINTZ K.E., JAKOBSSON P., JAPELJ J., KAPER L., TANVIR N.R., VREESWIJK P.M. and ZAFAR T.

Abstract (from CDS):


Context. Damped Lyman-α (DLA) absorption-line systems at the redshifts of gamma-ray burst (GRB) afterglows offer a unique way to probe the physical conditions within star-forming galaxies in the early Universe.
Aims. Here we built up a large sample of 22 GRBs at redshifts z>2 observed with VLT/X-shooter in order to determine the abundances of hydrogen, metals, dust, and molecular species. This allows us to study the metallicity and dust depletion effects in the neutral interstellar medium at high redshift and to answer the question of whether (and why) there might be a lack of H2 in GRB-DLAs.
Methods. We developed new methods based on the Bayesian inference package, PyMC, to FIT absorption lines and measure the column densities of different metal species as well as atomic and molecular hydrogen. The derived relative abundances are used to FIT dust depletion sequences and determine the dust-to-metals ratio and the host-galaxy intrinsic visual extinction. Additionally, we searched for the absorption signatures of vibrationally-excited H2 and carbon monoxide.
Results. We find that there is no lack of H2-bearing GRB-DLAs. We detect absorption lines from molecular hydrogen in 6 out of 22 GRB afterglow spectra, with molecular fractions ranging between f~=5x10–5 and f~=0.04, and claim tentative detections in three additional cases. For the remainder of the sample, we measure, depending on S/N, spectral coverage and instrumental resolution, more or less stringent upper limits. The GRB-DLAs in our sample have on average low metallicities, [X/H]~=-1.3, comparable to the population of extremely-strong QSO-DLAs (logN(HI)>21.5). Furthermore, H2-bearing GRB-DLAs are found to be associated with significant dust extinction, AV>0.1mag, and dust-to-metals ratios DTM>0.4, confirming the importance of dust grains for the production of molecules. All these systems exhibit neutral hydrogen column densities log N(HI)>21.7. The overall fraction of H2 detections in GRB-DLAs is ≥27% (41% including tentative detections), which is three to four times larger than in the general QSO-DLA population. For 2<z<4, and considering column densities log N(HI)>21.7, the H2 detection fraction is 60-80% in GRB-DLAs and in extremely strong QSO-DLAs. This is likely due to the fact that both GRB- and QSO-DLAs with high neutral hydrogen column densities are probed by sight-lines with small impact parameters, indicating that the absorbing gas is associated with the inner regions of the absorbing galaxy, where the gas pressure is higher and the conversion of HI to H2 takes place.In the case of GRB hosts, this diffuse molecular gas is located at distances ≥500pc from the GRB and hence is unrelated to the star-forming region where the event occurred.

Abstract Copyright: © ESO 2019

Journal keyword(s): ISM: abundances - dust, extinction - ISM: molecules - techniques: spectroscopic - galaxies: high-redshift

Simbad objects: 39

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Number of rows : 39
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 121201A gB 00 53 52.21 -42 56 34.5           ~ 40 0
2 Fermi bn100728439 gB 02 56 13.44 +00 16 51.6           ~ 121 0
3 GRB 111008A gB 04 01 48.220 -32 42 34.09           ~ 103 0
4 GRB 121024A gB 04 41 53.31 -12 17 26.1           ~ 120 0
5 GRB 151027B gB 05 04 52.67 -06 27 00.7           ~ 49 0
6 Fermi bn120119170 gB 08 00 06.940 -09 04 53.83           ~ 159 0
7 Fermi bn111107035 gB 08 37 54.66 -66 31 12.3           ~ 82 0
8 GRB 130408A gB 08 57 37.30 -32 21 38.9           ~ 82 0
9 GRB 141109A gB 09 38 07.40 -00 36 28.6           ~ 56 0
10 GRB 170202A gB 10 10 06 +05 01.0           ~ 64 0
11 GRB 100219A gB 10 16 48.48 -12 34 00.0           ~ 112 0
12 GRB 180325A gB 10 29 42.57 +24 27 48.7           ~ 57 0
13 GRB 160203A gB 10 47 48.32 -24 47 20.4           ~ 40 0
14 Fermi bn120712571 gB 11 18 21.16 -20 02 01.1           ~ 69 0
15 GRB 140515A gB 12 24 15.48 +15 06 17.7           ~ 73 0
16 GRB 121229A gB 12 40 23.41 -50 35 37.2           ~ 51 0
17 Fermi bn110128073 gB 12 55 35.10 +28 03 54.1           ~ 71 0
18 GRB 080607A gB 12 59 47.14 +15 55 09.6           ~ 235 0
19 GRB 060206 gB 13 31 43.420 +35 03 03.60   19.99 17.09     ~ 313 0
20 GRB 140311A gB 13 57 13.29 +00 38 31.7           ~ 69 0
21 GRB 050730 gB 14 08 17.090 -03 46 18.90   20.32 17.68     ~ 313 0
22 GRB 140614A gB 15 24 40.69 -79 07 43.8           ~ 33 0
23 GRB 120404A gB 15 40 02.29 +12 53 06.3           ~ 84 0
24 GRB 120327A gB 16 27 27.49 -29 24 53.8           ~ 95 0
25 GRB 130606A gB 16 37 35.12 +29 47 46.4           ~ 154 0
26 Fermi bn130612141 gB 17 19 10.63 +16 43 11.8           ~ 75 0
27 GRB 120815A gB 18 15 54.40 -52 07 29.0           ~ 85 0
28 GRB 120909A gB 18 22 56.81 -59 26 54.9           ~ 82 0
29 Fermi bn140506880 gB 18 27 06.04 -55 38 08.7           ~ 84 0
30 GRB 161023A gB 20 44 05.20 -47 39 48.7           ~ 40 0
31 GRB 150403A gB 20 46 01.17 -62 42 40.1           ~ 85 0
32 Fermi bn120716712 gB 20 52 12.17 +09 35 53.9           ~ 63 0
33 GRB 130427B gB 20 59 36.00 -22 32 51.6           ~ 49 0
34 GRB 141028A gB 21 30 24.46 -00 13 55.6           ~ 92 0
35 GRB 090809 gB 21 54 43.2 -00 05 02           ~ 78 0
36 GRB 131117A gB 22 09 19.47 -31 45 44.5           ~ 56 0
37 GRB 161014A gB 22 10 35.42 +07 28 07.6           ~ 51 0
38 GRB 151021A gB 22 30 34.43 -33 11 50.4           ~ 54 0
39 Fermi bn090926181 gB 23 33 36.18 -66 19 25.9           ~ 303 0

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