The Monte Carlo generators produce the final four vectors of all the particles
in the main process. However the quarks and leptons fragment into
showers of particles. To model this
process and also Final State Radiation (FSR), hadronisation programs are
employed. There are two main
fragmentation schemes used at OPAL; JETSET [84] which is
the fragmentation scheme from PYTHIA, and the HERWIG fragmentation scheme.
Both these hadronisation programs have been tuned using data measured at
OPAL [88,89] to give the best representation of true fragmentation.