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After the result of GRB970508 no more redshift has
been measured on the GRB optical transient itself
but 3 redshift have been measured of an host object overimposed to the transient itself. Of course while
the association of the absorption features of
GRB970508 provides an unambiguous lower limit to
the distance, the association of the GRB to each individual host is less compelling. The probability
of a random association is in average of the order
of 1% even if data come from instruments used at
the limit of sensitivity and to be compared with
a relatively poor statistics. Since in more than 3/4
of the cases optical transient are associated to a (slightly) extended object the following list is
very likely true.
Ordering by the redshift:
- GRB970508: z=0.835
- GRB980703: z=0.964
- GRB980613: z=1.096
- GRB971214: z=3.418
The result on GRB971214 is the most impressive since, assuming an isotropic emission (no beaming), it
corresponds to a significant fraction of a solar mass (around 0.3) converted into electromagnetic energy in
the 40-700 keV band. The impact of this datum was high. Until that date the most popular model for the
"central engine" was the merging of a Neutron Star-Neutron Star binary system. The energy of GRB971214
requires a beaming if the emission is originated in this way, but this makes unlikely the observed rate of GRBs. Moreover,
the optical transients, when imaged at high resolution, are usually in the central regions of their nebular
hosts while the expectation on runaway velocity of
binary systems including a collapsed object, combined
with the long time required for the merging, makes more likely a location external to the galaxy at the moment of the collapse.
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Lorenzo Amati
8/30/1999