Evidence for a canonical gamma-ray burst afterglow light curve in the Swift XRT data

被引:780
作者
Nousek, JA [1 ]
Kouveliotou, C
Grupe, D
Page, KL
Granot, J
Ramirez-Ruiz, E
Patel, SK
Burrows, DN
Mangano, V
Barthelmy, S
Beardmore, AP
Campana, S
Capalbi, M
Chincarini, G
Cusumano, G
Falcone, AD
Gehrels, N
Giommi, P
Goad, MR
Godet, O
Hurkett, CP
Kennea, JA
Moretti, A
O'Brien, PT
Osborne, JP
Romano, P
Tagliaferri, G
Wells, AA
机构
[1] Penn State Univ, Dept Astron & Astrophys, University Pk, PA 16802 USA
[2] Natl Space Sci Technol Ctr, NASA, George C Marshall Space Flight Ctr, Huntsville, AL 35805 USA
[3] Univ Leicester, Dept Phys & Astron, Leicester LE1 7RH, Leics, England
[4] Stanford Univ, Kavli Inst Particle Astrophys & Cosmol, Stanford, CA 94309 USA
[5] Inst Adv Study, Princeton, NJ 08540 USA
[6] Univ Space Res Assoc, MSFC, NASA, IPA, Columbia, MD 21044 USA
[7] Ist Fis Spazialee Fis Cosm, Sez Palermo, INAF, Palermo, Italy
[8] NASA, Goddard Space Flight Ctr, Greenbelt, MD 20771 USA
[9] Osserv Astron Brera, INAF, Merate, Italy
[10] ASI Sci Data Ctr, Frascati, Italy
[11] Univ Milan, Dipartimento Fis, Milan, Italy
关键词
gamma rays : bursts; radiation mechanisms : nonthermal;
D O I
10.1086/500724
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
We present new observations of the early X-ray afterglows of the first 27 gamma-ray bursts (GRBs) well observed by the Swift X-Ray Telescope (XRT). The early X-ray afterglows show a canonical behavior, where the light curve broadly consists of three distinct power-law segments: (1) an initial very steep decay (alpha(t-alpha) with 3 less than or similar to alpha(1) less than or similar to 5), followed by (2) a very shallow decay (0:5P less than or similar to alpha(2) less than or similar to 1.0), and finally ( 3) a somewhat steeper decay (1 less than or similar to alpha(3) less than or similar to 1.5). These power-law segments are separated by two corresponding break times, t(break,1) less than or similar to 500 s and 10(3) s less than or similar to t(break,2) less than or similar to 10(4) s. On top of this canonical behavior, many events have superimposed X-ray flares, which are most likely caused by internal shocks due to long-lasting sporadic activity of the central engine, up to several hours after the GRB. We find that the initial steep decay is consistent with it being the tail of the prompt emission, from photons that are radiated at large angles relative to our line of sight. The first break in the light curve (t(break,1)) takes place when the forward shock emission becomes dominant, with the intermediate shallow flux decay (alpha 2) likely caused by the continuous energy injection into the external shock. When this energy injection stops, a second break is then observed in the light curve (t(break,2)). This energy injection increases the energy of the afterglow shock by at least a factor of f greater than or similar to 4 and augments the already severe requirements for the efficiency of the prompt gamma-ray emission.
引用
收藏
页码:389 / 400
页数:12
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