2004ApJ...608..846S


Query : 2004ApJ...608..846S

2004ApJ...608..846S - Astrophys. J., 608, 846-864 (2004/June-3)

Absorption in gamma-ray burst afterglows.

STRATTA G., FIORE F., ANTONELLI L.A., PIRO L. and DE PASQUALE M.

Abstract (from CDS):

We studied the X-ray and optical absorption properties of 13 gamma-ray burst (GRB) afterglows observed by BeppoSAX. We found that X-ray absorption in addition to the Galactic one along the line of sight is highly statistically significant in the two cases with the best statistics (probability >99.9%). In three other cases the presence of X-ray absorption is marginally significant (probability ∼97%). Measured rest-frame equivalent column densities of hydrogen, NH, range from 0.1x1022 to 10.0x1022/cm2 (at 90% confidence level) assuming a solar metal abundance. X-ray absorption may be common, although the quality of present data does not allow us to reach a firm conclusion. We found that the rest-frame column densities derived from XMM and Chandra data as quoted in the literature are in good agreement with the BeppoSAX estimated rest-frame NHrange, supporting our result. For the same GRB afterglow sample we evaluated the rest-frame visual extinction AVr. We fitted the optical-NIR afterglow photometry with a power-law model corrected at short wavelengths by four different extinction curves. By comparing X-ray absorptions and optical extinction, we found that if a Galactic-like dust grain size distribution is assumed, a dust-to-gas ratio lower than the one observed in the Galaxy is required by the data. A dust-to-gas ratio ∼1/10 that of the Galactic one, as in the Small Magellanic Cloud (SMC) environment, has been tested using the SMC extinction curve, which produces good agreement between the best-fit NHand AVr. We note, however, that the best-fit NHvalues have been obtained by assuming solar metal abundances, while the metallicity of the SMC ISM is ~(1)/(8) the solar one (Pei (ref???)1992). If such low metallicity were assumed, the best-fit NHvalues would be higher by a factor of ∼7, providing a significant increase of the χ2. Alternative scenarios to explain simultaneously the optical and X-ray data involve dust with grain size distributions biased toward large grains. Possible mechanisms that can bring about such a grain size distribution are discussed.

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Journal keyword(s): ISM: Dust, Extinction - Gamma Rays: Bursts - X-Rays: General

Simbad objects: 18

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Number of rows : 18
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 NAME SMC G 00 52 38.0 -72 48 01   2.79 2.2     ~ 12317 1
2 GRB 000210 gB 01 59 15 -40 40.0           ~ 175 0
3 GRB 970228 gB 05 01 46.7 +11 46 53           ~ 650 1
4 M 1 SNR 05 34 31.8 +22 01 03           ~ 6516 1
5 V* CM Tau Psr 05 34 31.9474694616 +22 00 52.153698024           ~ 5476 0
6 GRB 970508 gB 06 53 49.2 +79 16 19           ~ 883 1
7 GRB 980329 gB 07 02 41 +38 50.7           ~ 276 1
8 SN 2003dh SN* 10 44 50.030 +21 31 18.15     16.2     SNIcpec 1261 1
9 GRB 971214 gB 11 56 26.4 +65 12 01           ~ 445 1
10 GRB 990704 gB 12 19 27.3 -03 50 22           ~ 50 0
11 GRB 990510 gB 13 38 07.64 -80 29 48.8           ~ 499 1
12 GRB 010222 G 14 52 12.5 +43 01 06           ~ 364 1
13 GRB 990123 gB 15 25 29 +44 45.0     8.95     ~ 1012 1
14 GRB 000926 gB 17 04 15 +51 46.0           ~ 373 0
15 GRB 001109 gB 18 30 07.8 +55 17 56           ~ 39 0
16 GRB 000214 gB 18 54 27.0 -66 27 30           ~ 92 0
17 GRB 980519 gB 23 22 21.5 +77 15 43           ~ 203 0
18 GRB 980703 gB 23 59 06.7 +08 35 07           ~ 453 1

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