2006A&A...460..105V


Query : 2006A&A...460..105V

2006A&A...460..105V - Astronomy and Astrophysics, volume 460105-116 (2006/12-2)

Forming a constant density medium close to long gamma-ray bursts.

VAN MARLE A.J., LANGER N., ACHTERBERG A. and GARCIA-SEGURA G.

Abstract (from CDS):

The progenitor stars of long Gamma-Ray Bursts (GRBs) are thought to be Wolf-Rayet stars, which generate a massive and energetic wind. Nevertheless, about 25 percent of all GRB afterglows light curves indicate a constant density medium close to the exploding star. We explore various ways to produce this, by creating situations where the wind termination shock arrives very close to the star, as the shocked wind material has a nearly constant density. Typically, the distance between a Wolf-Rayet star and the wind termination shock is too large to allow afterglow formation in the shocked wind material. Here, we investigate possible causes allowing for a smaller distance: A high density or a high pressure in the surrounding interstellar medium (ISM), a weak Wolf-Rayet star wind, the presence of a binary companion, and fast motion of the Wolf-Rayet star relative to the ISM. We find that all four scenarios are possible in a limited parameter space, but that none of them is by itself likely to explain the large fraction of constant density afterglows. A low GRB progenitor metallicity, and a high GRB energy make the occurrence of a GRB afterglow in a constant density medium more likely. This may be consistent with constant densities being preferentially found for energetic, high redshift GRBs.

Abstract Copyright: ∼

Journal keyword(s): stars: Wolf-Rayet - stars: winds, outflows - gamma rays: bursts - ISM: bubbles - hydrodynamics

Simbad objects: 22

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Number of rows : 22
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 021004 gB 00 26 54.68 +18 55 41.6           ~ 560 0
2 GRB 050904 gB 00 54 50.794 +14 05 09.42           ~ 496 0
3 GRB 970228 gB 05 01 46.7 +11 46 53           ~ 650 1
4 GRB 991216 gB 05 09 31.2983 +11 17 07.262           ~ 430 0
5 GRB 970508 gB 06 53 49.2 +79 16 19           ~ 883 1
6 HD 56925 WR* 07 18 29.1311435688 -13 13 01.513932528 11.21 11.74 11.56 11.40   WN4b 181 0
7 NGC 2359 HII 07 18 30.000 -13 13 36.00           ~ 170 0
8 SN 2002lt SN* 08 08 59.858 +06 43 37.52           SNIc: 363 1
9 V* V712 Car EB* 10 23 58.0126366512 -57 45 48.937268268 15.466 15.473 13.5 12.6   O3If*/WN6+O3If*/WN6 176 0
10 HD 96548 WR* 11 06 17.2032351624 -65 30 35.241182028 7.10 7.80 7.70 8.49   WN8h 427 0
11 GRB 011121 gB 11 34 26.67 -76 01 41.6       23.0   ~ 286 1
12 GRB 000418 gB 12 25 21 +20 05.0           ~ 219 0
13 GRB 990510 gB 13 38 07.64 -80 29 48.8           ~ 499 1
14 GRB 020405 gB 13 58 03.12 -31 22 22.2   21.9 21.5     ~ 259 1
15 GRB 010222 G 14 52 12.5 +43 01 06           ~ 364 1
16 GRB 990123 gB 15 25 29 +44 45.0     8.95     ~ 1012 1
17 GRB 000301C gB 16 20 18.5 +29 26 35           ~ 361 0
18 GRB 991208 gB 16 33 53.51 +46 27 21.5           ~ 269 1
19 GRB 000926 gB 17 04 15 +51 46.0           ~ 373 0
20 Hen 2-427 WR* 19 11 30.8749167768 +16 51 38.200938264   12.19 11.50     WN8h 350 0
21 HD 192163 WR* 20 12 06.5418877464 +38 21 17.784181008 7.12 7.49 7.50     WN6(h)-s 715 1
22 GRB 980703 gB 23 59 06.7 +08 35 07           ~ 453 1

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