The puzzling case of GRB 990123: prompt emission and broad-band afterglow modeling

被引:37
作者
Corsi, A
Piro, L
Kuulkers, E
Amati, L
Antonelli, LA
Costa, E
Feroci, M
Frontera, F
Guidorzi, C
Heise, J
Zand, JI
Maiorano, E
Montanari, E
Nicastro, L
Pian, E
Soffitta, P
机构
[1] IASF, CNR, I-00133 Rome, Italy
[2] Univ Roma La Sapienza, I-00185 Rome, Italy
[3] ESA, ESTEC, Sci Operat & Data Syst Div, SCI,SDG, NL-2201 AZ Noordwijk, Netherlands
[4] IASF, CNR, I-40129 Bologna, Italy
[5] Rome Astron Observ, I-00044 Frascati, Italy
[6] Univ Ferrara, Dept Phys, I-00044 Frascati, Italy
[7] Space Res Org Netherlands, NL-3584 CA Utrecht, Netherlands
[8] Univ Bologna, Dept Astron, I-40126 Bologna, Italy
[9] CNR, IASF, I-90146 Palermo, Italy
[10] Osserv Astron Trieste, INAF, I-34131 Trieste, Italy
关键词
gamma rays : bursts; X-rays : bursts; radiation mechanisms : non-thermal; cosmology : observations;
D O I
10.1051/0004-6361:20042532
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
We report on BeppoSAX simultaneous X-and gamma-ray observations of the bright gamma-ray burst (GRB) 990123. We present the broad-band spectrum of the prompt emission, including optical, X- and gamma-rays, confirming the suggestion that the emission mechanisms at low and high frequencies must have different physical origins. In the framework of the standard fireball model, we discuss the X- ray afterglow observed by the Narrow Field Instruments (NFIs) on board BeppoSAX and its hard X- ray emission up to 60 keV several hours after the burst, detected for about 20 ks by the Phoswich Detection System (PDS). Considering the 2-10 keV and optical light curves, the 0.1-60 keV spectrum during the 20 ks in which the PDS signal was present and the 8.46 GHz upper limits, we find that the multi-wavelength observations cannot be readily accommodated by basic afterglow models. While the temporal and spectral behavior of the optical afterglow is possibly explained by a synchrotron cooling frequency between the optical and the X- ray energy band during the NFIs observations, in X- rays this assumption only accounts for the slope of the 2-10 keV light curve, but not for the flatness of the 0.1-60 keV spectrum. Including the contribution of Inverse Compton (IC) scattering, we solve the problem of the flat X- ray spectrum and justify the hard X- ray emission; we also suggest that the lack of a significant detection of 15-60 keV emission in the following 75 ks and last 70 ks spectra, should be related to poorer statistics rather than to an important suppression of IC contribution. However, considering also the radio band data, we find the 8.46 GHz upper limits violated. On the other hand, leaving unchanged the emission mechanism requires modifying the hydrodynamics by invoking an ambient medium whose density rises rapidly with radius and by having the shock losing energy. Thus we are left with an open puzzle which requires further inspection.
引用
收藏
页码:829 / U31
页数:16
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