2024A&A...690A.373R


Query : 2024A&A...690A.373R

2024A&A...690A.373R - Astronomy and Astrophysics, volume 690A373 (2024/10-1)

A simple model of dust extinction in gamma-ray burst host galaxies.

RAKOTONDRAINIBE N.A., BUAT V., TURPIN D., DORNIC D., LE FLOC'H E., VERGANI S.D. and BASA S.

Abstract (from CDS):

Context. Gamma-ray burst (GRB) afterglows are powerful probes for studying the different properties of their host galaxies (e.g., the interstellar dust) at all redshifts. By fitting their spectral energy distribution (SED) over a large range of wavelengths, we can gain direct insights into the properties of the interstellar dust by studying the extinction curves. Unlike the dust extinction templates, such as those of the average Milky Way (MW) or the Small and Large Magellanic Cloud (SMC and LMC), the extinction curves of galaxies outside the Local Group exhibit deviation from these laws. Altogether, X-ray and gamma-ray satellites as well as ground-based telescopes, such as Neil Gehrels Swift Observatory (Swift) and Gamma-Ray Optical and Near-Infrared Detector (GROND), provide measurements of the afterglows from the X-ray to the NIR, which can be used to extract information on dust extinction curves along their lines of sight (LoS). The study presented in this paper undertakes such a photometric study, comprising a preparatory work for the SVOM mission and its ground-based follow-up telescope COLIBRI.
Aims. We propose a simple approach to parameterize the dust extinction curve of GRB host galaxies. The model used in this analysis is based on a power law form with the addition of a Loretzian-like Drude profile with two parameters: the extinction slope, γ, and the 2175 Å bump amplitude, Eb.
Methods. Using the g'r'i'z'JHKs GROND filter bands, we tested our dust extinction model and explored the parameter space in extinction and redshift by fitting SEDs of simplified simulations of GRB afterglow spectra based on different extinction curve templates. From a final sample of 10 real Swift/GROND extinguished GRBs, we determined the quantities of the dust extinction in their host and measured their extinction curves.
Results. We find that our derived extinction curves are in agreement with the spectroscopic measurements reported for four GRBs in the literature. We compared four other GRBs to the results of photometric studies where fixed laws were used to fit their data. We additionally derived two new GRB extinction curves. The measured average extinction curve is given by a slope of γ = 1.051 ± 0.129 and Eb = 0.070 ± 0.036, which is equivalent to a quasi-featureless in-between SMC-LMC template. This is consistent with previous studies aimed at deriving the dust host galaxy extinction where we expect that small dust grains dominate in GRB environment, yielding a steeper curve than the mean MW extinction curve.

Abstract Copyright: © The Authors 2024

Journal keyword(s): gamma-ray burst: general - dust - extinction

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 150206A gB 00 40 17.57 -63 10 56.0           ~ 55 0
3 GRB 070802 gB 02 27 35.91 -55 31 39.1           ~ 168 0
4 GRB 081230 gB 02 29 19.20 -25 08 42.6           ~ 50 0
5 GRB 081228 gB 02 37 50.80 +30 51 09.2           ~ 43 0
6 GRB 191011A gB 02 58 54.70 -27 50 43.4           ~ 38 0
7 NAME Magellanic Clouds GrG 03 00 -71.0           ~ 7988 0
8 GRB 111008A gB 04 01 48.220 -32 42 34.09           ~ 127 0
9 Fermi bn170113420 gB 04 06 59 -71 56.0           ~ 64 0
10 GRB 121027A gB 04 14 23.450 -58 49 47.17           ~ 136 0
11 GRB 121024A gB 04 41 53.31 -12 17 26.1           ~ 143 0
12 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 19090 0
13 GRB 081118 gB 05 30 22.28 -43 18 03.1           ~ 79 0
14 RMC 136 Cl* 05 38 42.396 -69 06 03.36   5.81 5.40     ~ 2236 2
15 Fermi bn150301818 gB 05 56 40.04 -57 58 10.4           ~ 67 0
16 GRB 081121 gB 05 57 07.70 -60 36 42.1           ~ 152 0
17 Fermi bn120119170 gB 08 00 06.940 -09 04 53.83           ~ 193 0
18 GRB 081028 gB 08 07 34.40 +02 18 16.8           ~ 125 0
19 GRB 090102 gB 08 32 59.50 +33 06 25.7           ~ 253 0
20 Fermi bn090516353 gB 09 12 59 -11 50.9           ~ 173 0
21 GRB 100219A gB 10 16 48.48 -12 34 00.0           ~ 130 0
22 GRB 180325A gB 10 29 42.57 +24 27 48.7           ~ 85 0
23 GRB 160203A gB 10 47 48.32 -24 47 20.4           ~ 54 0
24 Fermi bn120712571 gB 11 18 21.16 -20 02 01.1           ~ 90 0
25 GRB 090426 G 12 36 18.0470 +32 59 09.460           ~ 237 0
26 GRB 140428A gB 12 57 28.45 +28 23 05.7           ~ 35 0
27 GRB 140311A gB 13 57 13.29 +00 38 31.7           ~ 86 0
28 GRB 090205 gB 14 43 40.00 -27 50 51.4           ~ 99 0
29 GRB 140614A gB 15 24 40.69 -79 07 43.8           ~ 43 0
30 Fermi bn120922939 gB 15 38 59.67 -20 10 55.0           ~ 88 0
31 GRB 120404A gB 15 40 02.29 +12 53 06.3           ~ 104 0
32 GRB 130606A gB 16 37 35.12 +29 47 46.4           ~ 185 0
33 GRB 080210 gB 16 45 04.03 +13 49 36.3           ~ 121 0
34 GRB 080605 gB 17 28 30.04 +04 00 56.9           ~ 198 0
35 HD 164340 bC* 18 02 32.9452043448 -40 05 16.419321528 8.2 9.16 9.25     B0/0.5(III) 46 0
36 GRB 120815A gB 18 15 54.40 -52 07 29.0           ~ 103 0
37 Fermi bn110731465 gB 18 42 00.99 -28 32 13.8           ~ 193 0
38 GRB 020813A gB 19 46 41.874 -19 36 04.81           ~ 316 0
39 GRB 161023A gB 20 44 05.20 -47 39 48.7           ~ 49 0
40 GRB 080514B gB 21 31 22.61 +00 42 30.3           ~ 69 0
41 HD 210121 * 22 08 11.9027578440 -03 31 52.765490316   7.84 7.68     B7II 185 0
42 GRB 131117A gB 22 09 19.47 -31 45 44.5           ~ 67 0
43 HD 211021 * 22 14 30.6840485856 -12 15 13.478874768   8.93 8.09     G8V 12 0
44 GRB 081029 gB 23 07 06 -68 10.7           ~ 121 0
45 GRB 090812 gB 23 32 48.5 -10 36 17           ~ 165 0
46 GRB 901021 gB ~ ~           ~ 2 0
47 NAME Local Group GrG ~ ~           ~ 9325 0

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