2021A&A...653A..83V


Query : 2021A&A...653A..83V

2021A&A...653A..83V - Astronomy and Astrophysics, volume 653A83-83 (2021/9-1)

Gamma-ray bursts as probes of high-redshift Lyman-α emitters and radiative transfer models.

VIELFAURE J.-B., VERGANI S.D., GRONKE M., JAPELJ J., PALMERIO J.T., FYNBO J.P.U., MALESANI D.B., MILVANG-JENSEN B., SALVATERRA R. and TANVIR N.R.

Abstract (from CDS):


Aims. We present the updated census and statistics of Lyman-α emitting long gamma-ray burst host galaxies (LAE-LGRBs). We investigate the properties of a subsample of LAE-LGRBs and test the shell model that is commonly used to fit Lyman-α (Lyα) emission line spectra.
Methods. We considered all LGRB host galaxies with relevant publicly available information. We defined a golden sample of four LAE-LGRBs (GRBs 011211, 021004, 060926, and 070110) with afterglow and host galaxy observations allowing us to constrain the shell modeling of the Lyα line.
Results. The census results in 29 detected LAE-LGRBs. We present 5 new Lyα emission detections in host-galaxy spectra and the corresponding unpublished VLT/X-shooter data (GRBs 060926, 070110, 081121, 081222, and 100424A). From the comparison of the statistics and properties of LAE-LGRBs to those of LAE samples in the literature, we find evidence of Lyα suppression in dusty systems. The fraction of LAE-LGRBs in the overall LGRB hosts is lower than that found for Lyman-break galaxy (LBG) samples at similar redshift range. This result can arise because the selection criteria of the parent samples are different and the spectral observations of LGRB samples are shallower than those of LBG. However, we find that LAE-LGRBs are representative of Lyα emission from the bulk of UV-selected galaxies at z∼2. We find that the golden sample of LAE-LGRBs we studied consists of complex systems characterized by multiple emission blobs and by signs of possible galaxy interactions. The fitting procedure recovers the HI column densities (NHI) measured from the afterglow spectra and the other properties described by the shell-model parameters in the two low-NHI cases, but it fails to do this in the other two cases with high NHI. The afterglows of most LGRBs and LAE-LGRBs show log(NHI/cm–2)>20.3, implying that statistically, the bulk of Lyα photons that is expected to be produced by massive stars in the star-forming region hosting the GRB will be surrounded by these opaque lines of sight. We therefore interpret our results in the context of more sophisticated models and of different dominant Lyα-emitting regions. We also compare LAE-LGRBs to LAE Lyman continuum (LyC) leakers in the literature in terms of the properties that are identified as possible indirect indicators of LyC leakage. We find that only one LGRB (GRB 021004) would likely be a strong LyC leaker and discuss the validity of these indicators at high redshift. While our work shows that LGRBs are useful tools for probing LAEs and radiative transfer models, larger statistics are required to strengthen our findings.

Abstract Copyright: © J.-B. Vielfaure et al. 2021

Journal keyword(s): gamma-ray burst: general - galaxies: star formation - galaxies: ISM - galaxies: evolution - galaxies: high-redshift - line: profiles

VizieR on-line data: <Available at CDS (J/A+A/653/A83): list.dat sp/*>

Simbad objects: 76

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Number of rows : 76
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 121201A gB 00 53 52.21 -42 56 34.5           ~ 49 0
6 GRB 050904 gB 00 54 50.794 +14 05 09.42           ~ 496 0
7 Fermi bn081221681 gB 01 03 10.2 -24 32 53           ~ 186 0
8 GRB 080602 gB 01 16 42.18 -09 13 55.4           ~ 61 0
9 GRB 050908 gB 01 21 50.750 -12 57 17.20           ~ 179 0
10 GRB 081222 gB 01 30 57.76 -34 05 44.0           ~ 199 0
11 GRB 060908 gB 02 07 18.360 +00 20 31.20 16.99 18.34 16.85     ~ 217 0
12 Fermi bn090113778 gB 02 08 16.00 +33 26 08.4           ~ 92 0
13 GRB 070721B gB 02 12 32.98 -02 11 39.8           ~ 128 0
14 GRB 070802 gB 02 27 35.91 -55 31 39.1           ~ 168 0
15 GRB 070129 gB 02 28 00.940 +11 41 04.00       21.3   ~ 120 0
16 GRB 191004B gB 03 16 48.97 -39 38 06.3           ~ 32 0
17 GRB 060115 gB 03 36 08.400 +17 20 43.00           ~ 179 0
18 GRB 070328 gB 04 20 27.680 -34 04 00.60 20.29         ~ 97 0
19 GRB 081210 gB 04 41 56.19 -11 15 27.8           ~ 56 0
20 GRB 050915A gB 05 26 44.804 -28 00 59.27           ~ 88 0
21 GRB 081121 gB 05 57 07.70 -60 36 42.1           ~ 152 0
22 GRB 090201 gB 06 08 12.30 -46 36 16.1           ~ 68 0
23 GRB 061202 gB 07 02 06.190 -74 41 54.91           ~ 83 0
24 Fermi bn120119170 gB 08 00 06.940 -09 04 53.83           ~ 193 0
25 Fermi bn120118709 gB 08 19 29.05 -07 11 05.1           ~ 87 0
26 Fermi bn090423330 gB 09 55 33.19 +18 08 57.7           ~ 392 0
27 GRB 170202A gB 10 10 06 +05 01.0           ~ 90 0
28 GRB 070223 gB 10 13 48.390 +43 08 00.71 21.47         ~ 67 0
29 GRB 111123A gB 10 19 23.17 -20 38 41.9           ~ 83 0
30 GRB 030323 gB 11 06 09.4 -21 46 13           ~ 138 1
31 GRB 011211 gB 11 15 16 -21 56.0           ~ 305 0
32 GRB 050714B gB 11 18 47.610 -15 32 48.90           ~ 80 0
33 Fermi bn120624933 gB 11 23 31.98 +08 55 42.1           ~ 100 0
34 GRB 130131B gB 11 35 49.60 +15 01 59.3           ~ 51 0
35 GRB 070224 gB 11 56 06.650 -13 19 48.80           ~ 60 0
36 GRB 971214 gB 11 56 26.4 +65 12 01           ~ 445 1
37 GRB 030429 gB 12 13 07.495 -20 54 49.54     23.70     ~ 132 0
38 Fermi bn090323002 gB 12 42 50.28 +17 03 11.9           ~ 244 1
39 GRB 080207 gB 13 50 03.02 +07 30 08.0           ~ 114 0
40 GRB 100424A gB 13 57 47.46 +01 32 20.3           ~ 71 0
41 GRB 060204B gB 14 07 14.900 +27 40 36.40           ~ 93 0
42 GRB 050730 gB 14 08 17.090 -03 46 18.90   20.32 17.68     ~ 327 0
43 GRB 090205 gB 14 43 40.00 -27 50 51.4           ~ 99 0
44 GRB 060805A gB 14 43 43.480 +12 35 11.40           ~ 65 0
45 GRB 060814 gB 14 45 21.480 +20 35 11.80           ~ 241 0
46 GRB 060714 gB 15 11 26.450 -06 33 58.30   20.21 18.54     ~ 209 0
47 GRB 060526 gB 15 31 18.360 +00 17 04.90   18.31 17.16     ~ 288 0
48 GRB 070521 gB 16 10 38.600 +30 15 22.70           ~ 164 0
49 GRB 050401 gB 16 31 28.84 +02 11 14.5           ~ 348 0
50 GRB 100316A gB 16 47 55.56 +71 49 40.0           ~ 34 0
51 GRB 000926 gB 17 04 15 +51 46.0           ~ 373 0
52 GRB 080605 gB 17 28 30.04 +04 00 56.9           ~ 198 0
53 GRB 060926 gB 17 35 43.660 +13 02 18.60     19.36     ~ 135 0
54 GRB 120815A gB 18 15 54.40 -52 07 29.0           ~ 103 0
55 GRB 050315 gB 20 25 54.100 -42 36 02.19           ~ 225 0
56 GRB 070419B gB 21 02 49.820 -31 15 49.30   20.35       ~ 86 0
57 Fermi bn110818860 gB 21 09 20.890 -63 58 51.80           ~ 92 0
58 GRB 050922C gB 21 09 33.000 -08 45 30.10 15.15 15.86 14.69     ~ 301 0
59 GRB 150915A gB 21 18 37.88 -34 54 48.2           ~ 30 0
60 GRB 060605 gB 21 28 37.320 -06 03 31.30   20.12 16.53     ~ 210 0
61 GRB 060522 gB 21 31 44.850 +02 53 10.80           ~ 140 0
62 GRB 061110B gB 21 35 40.400 +06 52 34.10           ~ 91 0
63 Fermi bn080804972 gB 21 54 41.90 -53 11 20.2           ~ 158 0
64 GRB 060927A gB 21 58 11.930 +05 21 50.32           ~ 215 0
65 GRB 060607 gB 21 58 50.400 -22 29 46.70 18.49 16.67 15.09     ~ 318 0
66 GRB 060604 gB 22 28 55.010 -10 54 55.80 20.34 20.31       ~ 134 0
67 GRB 050820A gB 22 29 38.110 +19 33 37.10 18.33 19.00 18.47     ~ 409 0
68 GRB 151021A gB 22 30 34.43 -33 11 50.4           ~ 72 0
69 GRB 071021 gB 22 42 34.33 +23 43 05.4           ~ 104 0
70 GRB 070506 gB 23 08 52.390 +10 43 20.30     19.04     ~ 86 0
71 GRB 051001 gB 23 23 48.580 -31 31 25.70           ~ 80 0
72 GRB 070103 gB 23 30 13.750 +26 52 33.70           ~ 76 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
75 GRB 061222A gB 23 53 03.419 +46 31 58.60           ~ 177 0
76 GRB 050819 gB 23 55 01.650 +24 51 38.80           ~ 75 0

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