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  4. Swift XRT Observations of the Afterglow of XRF 050416A
 
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Swift XRT Observations of the Afterglow of XRF 050416A

Author(s)
Mangano, Vanessa
La Parola, Valentina
Cusumano, Giancarlo
Capalbi, Milvia
Giommi, Paolo  
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Subjects

Gamma Rays Bursts

X-rays individual (XR...

Date Issued
2007-01-01
Mission(s)
Swift  
Abstract
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 alpha~2.4), subsequently flattens (alpha~0.44), and eventually steepens again (alpha~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 Gamma~3.0 during the initial steep decay, to a harder emission with Gamma~2.0 during the following evolutionary phases. The spectra show intrinsic absorption in the host galaxy with column density of ~6.810<SUP>21</SUP> cm<SUP>-2</SUP>. 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.
URI
https://hdl.handle.net/20.500.13025/814
DOI
10.1086/509100
URL
http://adsabs.harvard.edu/abs/2007ApJ...654..403M
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