2007ApJ...654..403M


Query : 2007ApJ...654..403M

2007ApJ...654..403M - Astrophys. J., 654, 403-412 (2007/January-1)

Swift XRT observations of the afterglow of XRF 050416A.

MANGANO V., LA PAROLA V., CUSUMANO G., MINEO T., MALESANI D., DYKS J., CAMPANA S., CAPALBI M., CHINCARINI G., GIOMMI P., MORETTI A., PERRI M., ROMANO P., TAGLIAFERRI G., BURROWS D.N., GEHRELS N., GODET O., HOLLAND S.T., KENNEA J.A., PAGE K.L., RACUSIN J.L., ROMING P.W.A. and ZHANG B.

Abstract (from CDS):

Swift discovered XRF 050416A with the Burst Alert Telescope and began observing it with its narrow-field instruments only 64.5 s after the burst onset. Its very soft spectrum classifies this event as an X-ray flash. The afterglow X-ray emission was monitored up to 74 days after the burst. The X-ray light curve initially decays very fast (decay slope α∼2.4), subsequently flattens (α∼0.44), and eventually steepens again (α∼0.88), similar to many X-ray afterglows. The first and second phases end ∼172 and ∼1450 s after the burst onset, respectively. We find evidence of spectral evolution from a softer emission with photon index Γ∼3.0 during the initial steep decay, to a harder emission with Γ∼2.0 during the following evolutionary phases. The spectra show intrinsic absorption in the host galaxy with column density of ∼6.8x1021/cm2. The consistency of the initial photon index with the high-energy BAT photon index suggests that the initial fast decaying phase of the X-ray light curve may be the low-energy tail of the prompt emission. The lack of jet break signatures in the X-ray afterglow light curve is not consistent with empirical relations between the source rest-frame peak energy and the collimation-corrected energy of the burst. The standard uniform jet model can give a possible description of the XRF 050416A X-ray afterglow for an opening angle larger than a few tens of degrees, although numerical simulations show that the late-time decay is slightly flatter than expected from on-axis viewing of a uniform jet. A structured Gaussian-type jet model with uniform Lorentz factor distribution and viewing angle outside the Gaussian core is another possibility, although a full agreement with data is not achieved with the numerical models explored.

Abstract Copyright: ∼

Journal keyword(s): Gamma Rays: Bursts - X-rays: individual (XRF 050416A)

Simbad objects: 15

goto Full paper

goto View the references in ADS

Number of rows : 15
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 050824 gB 00 48 56.100 +22 36 32.00 19.66 21.03 20.46 23.70   ~ 184 0
2 GRB 050406 gB 02 17 52.200 -50 11 15.81     18.83     ~ 125 0
3 GRB 050318 gB 03 18 51.000 -46 23 43.61 18.10 18.68 17.58     ~ 189 0
4 GRB 050505 gB 09 27 03.300 +30 16 23.70     20.74     ~ 206 0
5 GRB 050502B gB 09 30 10.024 +16 59 48.07           ~ 169 0
6 GRB 050319 gB 10 16 47.900 +43 32 53.80   18.02 17.01     ~ 274 0
7 GRB 050215B gB 11 37 48.030 +40 47 43.39           ~ 71 0
8 GRB 050416 gB 12 33 54.600 +21 03 26.69     19.12     ~ 300 1
9 SN 2005nc SN* 18 32 32.560 +26 20 22.34           SNIc: 400 1
10 GRB 050607 gB 20 00 42.790 +09 08 31.50   19.55 18.94     ~ 103 0
11 GRB 050315 gB 20 25 54.100 -42 36 02.19           ~ 225 0
12 GRB 011030 gB 20 43 35.4 +77 17 20           ~ 76 0
13 GRB 040701 G 20 47 46.3 -40 14 13           ~ 45 1
14 GRB 030723 gB 21 49 24.40 -27 42 47.4           ~ 130 0
15 GRB 020427 gB 22 09 28.3 -65 19 32           ~ 50 0

To bookmark this query, right click on this link: simbad:objects in 2007ApJ...654..403M and select 'bookmark this link' or equivalent in the popup menu