2018A&A...609A..62B


Query : 2018A&A...609A..62B

2018A&A...609A..62B - Astronomy and Astrophysics, volume 609A62-62 (2018/1-1)

Dust reddening and extinction curves toward gamma-ray bursts at z> 4.

BOLMER J., GREINER J., KRUHLER T., SCHADY P., LEDOUX C., TANVIR N.R. and LEVAN A.J.

Abstract (from CDS):

Context. Dust is known to be produced in the envelopes of asymptotic giant branch (AGB) stars, the expanded shells of supernova (SN) remnants, and in situ grain growth within the interstellar medium (ISM), although the corresponding efficiency of each of these dust formation mechanisms at different redshifts remains a topic of debate. During the first Gyr after the Big Bang, it is widely believed that there was not enough time to form AGB stars in high numbers, hence the dust at this epoch is expected to be purely from SNe or subsequent grain growth in the ISM. The time period corresponding to z∼5-6 is thus expected to display the transition from SN-only dust to a mixture of both formation channels as is generally recognized at present.
Aims. Here we aim to use afterglow observations of gamma-ray bursts (GRBs) at redshifts larger than z>4 to derive host galaxy dust column densities along their line of sight and to test if a SN-type dust extinction curve is required for some of the bursts.
Methods. We performed GRB afterglow observations with the seven-channel Gamma-Ray Optical and Near-infrared Detector (GROND) at the 2.2m MPI telescope in La Silla, Chile (ESO), and we combined these observations with quasi-simultaneous data gathered with the XRT telescope on board the Swift satellite.
Results. We increase the number of measured AV values for GRBs at z>4 by a factor of ∼2-3 and find that, in contrast to samples at mostly lower redshift, all of the GRB afterglows have a visual extinction of AV<0.5mag. Analysis of the GROND detection thresholds and results from a Monte Carlo simulation show that although we partly suffer from an observational bias against highly extinguished sight-lines, GRB host galaxies at 4<z<6 seem to contain on average less dust than at z∼2. Additionally, we find that all of the GRBs can be modeled with locally measured extinction curves and that the SN-like dust extinction curve, as previously found toward GRB 071025, provides a better fit for only two of the afterglow SEDs. However, because of the lack of highly extinguished sight lines and the limited wavelength coverage we cannot distinguish between the different scenarios. For the first time we also report a photometric redshift of zphot=7.88–0.94+0.75 for GRB 100905A, making it one of the most distant GRBs known to date.

Abstract Copyright: © ESO, 2018

Journal keyword(s): galaxies: high-redshift - dust, extinction - techniques: photometric

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 151112A gB 00 08 12.84 -61 39 47.7           ~ 37 0
2 GRB 050922B gB 00 23 13.400 -05 36 17.80           ~ 79 0
3 NAME SMC G 00 52 38.0 -72 48 01   2.79 2.2     ~ 12317 1
4 GRB 050904 gB 00 54 50.794 +14 05 09.42           ~ 496 0
5 Fermi bn140304557 gB 02 02 33.90 +33 28 27.9           ~ 106 0
6 GRB 100905A gB 02 06 12.06 +14 55 45.9           ~ 45 0
7 GRB 060223A gB 03 40 49.560 -17 07 48.40     17.90     ~ 98 0
8 GRB 111008A gB 04 01 48.220 -32 42 34.09           ~ 127 0
9 GRB 080913 gB 04 22 57.90 -25 07 38.6           ~ 213 0
10 GRB 131227A gB 04 29 30.78 +28 52 59.2           ~ 35 0
11 GRB 151027B gB 05 04 52.67 -06 27 00.7           ~ 61 0
12 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 19090 0
13 GRB 090429A gB 06 02 13.28 -52 23 14.5           ~ 30 0
14 GRB 000131 gB 06 13 31.08 -51 56 41.7     24.7     ~ 172 1
15 GRB 080129 gB 07 01 08.13 -07 50 47.8           ~ 85 0
16 GRB 080916C gB 07 59 23.24 -56 38 16.8           ~ 386 0
17 Fermi bn090516353 gB 09 12 59 -11 50.9           ~ 173 0
18 GRB 050505 gB 09 27 03.300 +30 16 23.70     20.74     ~ 206 0
19 GRB 050502B gB 09 30 10.024 +16 59 48.07           ~ 169 0
20 GRB 070306 gB 09 52 23.220 +10 28 55.20           ~ 222 1
21 Fermi bn090423330 gB 09 55 33.19 +18 08 57.7           ~ 392 0
22 GRB 100219A gB 10 16 48.48 -12 34 00.0           ~ 130 0
23 Fermi bn120712571 gB 11 18 21.16 -20 02 01.1           ~ 90 0
24 GRB 100513A gB 11 18 26.83 +03 37 40.8           ~ 74 0
25 GRB 140515A gB 12 24 15.48 +15 06 17.7           ~ 90 0
26 GRB 140428A gB 12 57 28.45 +28 23 05.7           ~ 35 0
27 GRB 080607A gB 12 59 47.14 +15 55 09.6           ~ 257 0
28 GRB 100302A gB 13 02 03.66 +74 35 22.5           ~ 83 0
29 GRB 060206 gB 13 31 43.420 +35 03 03.60   19.99 17.09     ~ 330 0
30 GRB 080825B gB 13 56 48.2 -68 57 18           ~ 17 0
31 GRB 140311A gB 13 57 13.29 +00 38 31.7           ~ 86 0
32 GRB 090429B gB 14 02 40.10 +32 10 14.6           ~ 166 0
33 GRB 120521C gB 14 17 09.10 +42 08 39.8           ~ 93 0
34 GRB 090205 gB 14 43 40.00 -27 50 51.4           ~ 99 0
35 GRB 140518A gB 15 09 00.60 +42 25 05.6           ~ 68 0
36 GRB 140614A gB 15 24 40.69 -79 07 43.8           ~ 43 0
37 GRB 060510B gB 15 56 29.200 +78 34 12.00           ~ 155 0
38 GRB 130606A gB 16 37 35.12 +29 47 46.4           ~ 185 0
39 GRB 050814 gB 17 36 45.390 +46 20 21.60           ~ 166 0
40 GRB 090709A gB 19 19 46.70 +60 43 40.8           ~ 125 0
41 GRB 120923A gB 20 15 10.73 +06 13 16.9           ~ 59 0
42 GRB 100518A gB 20 19 09.330 -24 33 16.56           ~ 19 0
43 GRB 060522 gB 21 31 44.850 +02 53 10.80           ~ 140 0
44 GRB 060927A gB 21 58 11.930 +05 21 50.32           ~ 215 0
45 GRB 131117A gB 22 09 19.47 -31 45 44.5           ~ 67 0
46 GRB 071025 gB 23 40 17.02 +31 46 42.4           ~ 122 0
47 GRB 061222A gB 23 53 03.419 +46 31 58.60           ~ 177 0

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