G970508: A first epoch VLBA observation was obtained just 8 days
after the gamma-ray burst, and within 48 hours of the VLA discovery of
a radio counterpart (Frail et al. 1997a). An additional 8 epochs
were obtained until days after the burst when the radio
afterglow faded below 0.3 mJy,
the nominal sensitivity limit. From this data we derived a position
accurate to better than 0.1 mas, placed a 3
limit on the
proper motion of less than 5 mas y-1 and placed a limit on the parallax
of less than 0.3 mas corresponding to a distance limit of > 3 kpc
(Taylor et al. 1997;
Taylor et al. 1998). For all epochs the limit
on the angular size was less than 0.5 mas (<4 pc).
G980329: We observed, but did not detect, G980329, because variability drove it below 0.2 mJy on the day we observed. The radio afterglow from this source peaked below 0.5 mJy so we did not attempt further observations.
G980425:
Associated with SN1998bw in the galaxy ESO 184-G82 at
z=0.0083,
G980425 was studied with the ATCA during the first 60 days of its
outburst
(Kulkarni et al. 1998) and both scintillation and brightness
temperature arguments predict a size of 0.1 mas
on day 16. This time
is near the peak in the radio light curve of 50 mJy
at 8.4 GHz.
Unfortunately, only limited VLBI observations were feasible for this
far southern declination () source. On May 10 we
observed G980425 at 22 GHz with the VLBA antenna at Mauna Kea and with
the 70 meter antenna of the Deep Space Network at Tidbinbilla. The
radio source was not detected above a 3
limit of 30 mJy. On
August 19 we observed with the same two telescopes but at 8.4 GHz and
employing phase-referencing to increase the coherence time. No source
was detected above a 3
limit of 2.5 mJy. An 8.4 GHz
observation by a southern hemisphere network of radio telescopes on
May 9th is still being analyzed.
G980519: No VLBI observation was attempted of this very faint radio afterglow.
G980703:
The radio afterglow from G980703 reached
1 mJy in the first two weeks after the burst. We detected G980703
at a level of 0.5 mJy 30 days after the burst, when it was already
in decline (Fig. 1). We place a limit on the angular size of
G980703 of <0.3 mas, and derive a position of
(J2000) = 23
59
06.
6661,
(J2000) = 8
35
07.
0939
with an uncertainty of 0.0007 arcsec in each coordinate.
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