2007ApJ...660L.101W


Query : 2007ApJ...660L.101W

2007ApJ...660L.101W - Astrophys. J., 660, L101-L104 (2007/May-2)

Very different X-Ray-to-optical column density ratios in γ-ray burst afterglows: ionization in GRB environments.

WATSON D., HJORTH J., FYNBO J.P.U., JAKOBSSON P., FOLEY S., SOLLERMAN J. and WIJERS R.A.M.J.

Abstract (from CDS):

We compare the H I column densities from Lyα absorption to the metal column densities from X-ray absorption in γ-ray burst (GRB) afterglows. Eight bursts of 17 entering the sample have significant extragalactic X-ray absorptions. Of these we find a range in metallicities from subsolar to a few hundred times the solar value. There is a complete lack of correlation between the X-ray and optical column densities. This, and the large range and extreme values of these ``metallicities'', suggests that the column densities derived by one or both methods are not a reliable indication of the true total column densities toward GRBs. Ionization of the GRB's gas cloud to large distances along the line of sight seems the most likely cause. From the lower limit on the total column density and the UV luminosity of the GRBs, we derive a maximum distance to the majority of the gas surrounding GRBs of ∼3 pc, suggesting that the gas probed by optical afterglow spectra is not the cloud in which the burst occurs. This is an encouraging result for the use of GRB optical afterglows as probes of the interstellar medium (ISM) in their host galaxies, as the ISM observed is less likely to be strongly affected by the GRB or its progenitor.

Abstract Copyright: ∼

Journal keyword(s): Gamma Rays: Bursts - Galaxies: Quasars: Absorption Lines - X-Rays: Galaxies - X-Rays: General

CDS comments: Parag. 4 : GRB 050111 is a misprint for GRB 051111

Simbad objects: 23

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Number of rows : 23
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 050904 gB 00 54 50.794 +14 05 09.42           ~ 496 0
2 GRB 050908 gB 01 21 50.750 -12 57 17.20           ~ 179 0
3 QSO B0235+1624 BLL 02 38 38.93010450 +16 36 59.2745528   16.46 15.50 15.92   ~ 1614 2
4 GRB 060906 gB 02 43 00.900 +30 21 42.12     19.84     ~ 147 0
5 GRB 060210 gB 03 50 57.370 +27 01 34.40   20.27       ~ 275 0
6 GRB 060124 gB 05 08 25.900 +69 44 26.98   18.91 17.35     ~ 280 0
7 M 1 SNR 05 34 31.8 +22 01 03           ~ 6516 1
8 V* CM Tau Psr 05 34 31.9474694616 +22 00 52.153698024           ~ 5476 0
9 GRB 050505 gB 09 27 03.300 +30 16 23.70     20.74     ~ 206 0
10 GRB 050319 gB 10 16 47.900 +43 32 53.80   18.02 17.01     ~ 274 0
11 GRB 060206 gB 13 31 43.420 +35 03 03.60   19.99 17.09     ~ 330 0
12 GRB 050730 gB 14 08 17.090 -03 46 18.90   20.32 17.68     ~ 327 0
13 GRB 060714 gB 15 11 26.450 -06 33 58.30   20.21 18.54     ~ 209 0
14 GRB 060526 gB 15 31 18.360 +00 17 04.90   18.31 17.16     ~ 288 0
15 GRB 060418 gB 15 45 42.600 -03 38 20.00 15.73 16.19 14.98     ~ 389 0
16 GRB 050401 gB 16 31 28.84 +02 11 14.5           ~ 348 0
17 GRB 060926 gB 17 35 43.660 +13 02 18.60     19.36     ~ 135 0
18 GRB 050922C gB 21 09 33.000 -08 45 30.10 15.15 15.86 14.69     ~ 301 0
19 GRB 060522 gB 21 31 44.850 +02 53 10.80           ~ 140 0
20 GRB 060607 gB 21 58 50.400 -22 29 46.70 18.49 16.67 15.09     ~ 318 0
21 GRB 050820A gB 22 29 38.110 +19 33 37.10 18.33 19.00 18.47     ~ 409 0
22 GRB 051111A gB 23 12 33.170 +18 22 28.80 19.77 20.08 19.50     ~ 223 0
23 GRB 060707 gB 23 48 19.000 -17 54 17.00     19.79     ~ 170 0

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