The SLC collides bunches of electrons and positrons accelerated in the
SLAC linac at a rate of 120 Hz. After colliding at energies
of 45.6 GeV each, the bunches are extracted and dumped.
For the 1993 run, the spatial extent of the bunches at the interaction point
was typically m vertically,
m
horizontally, and
m longitudinally[6]. The
transverse position of the SLC collision region was stable, with variations
of typically 5-10
m over time periods measured in hours.
The spatial location of the interaction point is determined accurately
in the transverse plane using tracks from hadronic decays [7].
A fit to a single point in the transverse plane is made using tracks from 30
successive events, in an iterative procedure. At each iteration, tracks that
significantly reduce the quality of the fit are removed. Typically the fit uses
about 300 tracks, and converges after a few iterations. The uncertainty in this
determination is
m for the 1993 data and
m for the
1992 data. Non-Gaussian tails in the interaction point distribution may be
represented conservatively by a second Gaussian with a standard deviation
of 100
m for 0.25%(0.5%) of the 1993 (1992) events.