A follow-up observation performed with the BeppoSAX NFIs started less than 10 hrs after the trigger and a weak, rapidly decaying X-ray source was detected (Nicastro et al. 1998a). The decay was not monotonic, but the low counting rate did not allow us to reconstruct a detailed light curve.
Figure 2 shows the 2-10 keV (MECS) flux decay and
three possible
power-law decay fits .It can be seen that constraining the fit to connect with the last part
of the WFC detected flux, gives a minimum decay slope
. On the other hand, if the first point
of the NFIs observation is not a peak superimposed to the monotonic
decay, then we have
. This can be considered
a maximum decay slope. It is realistic to suppose that the real
slope is close to
obtained excluding the
first NFIs point from the fit. In any case, this is the most rapid decay
for all the 13 GRB afterglows detected so far, typical
values ranging between
.
Spectral fitting of the 0.1-10 keV LECS+MECS data using an absorbed
power-law gave
a quite soft photon index of 2.8+0.6-0.5
and in the range
(see Fig. 3).
The 0.1-2 keV flux is
erg cm-2 s-1
while the 2-10 keV flux is
erg cm-2 s-1.
Further details are given in Nicastro et al. (1998b).
Optical observations, started as early as 8 hours
after the GRB, resulted in the detection of the afterglow
(OT) in bands.
The power-law decays in all these bands were all consistent with
.Deep observations performed
days after the
burst with the 6-m telescope of the SAO-RAS
revealed that at the position of the OT there is a faint object,
possibly a galaxy, of magnitude
(Sokolov et al. 1998b).
It is worth to note that for all 9 optically identified GRBs,
there are indications of the presence of an underlying host galaxy
(Hogg & Fruchter 1998;
Sokolov et al. 1998a).
The afterglow was also detected in the radio band by the VLA
(Frail et al. 1998) at
R.A. = 2322
,
Dec. =
(J2000,
).
This research is supported by the Italian Space Agency (ASI) and Consiglio Nazionale delle Ricerche (CNR). BeppoSAX is a major program of ASI with participation of the Netherlands Agency for Aerospace Programs (NIVR). All authors warmly thank the extraordinary teams of the BeppoSAX Scientific Operation Center and Operation Control Center for their enthusiastic support to the GRB program. K.H. is grateful to the US SAX Guest Investigator program for support.
Copyright The European Southern Observatory (ESO)