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Final-state showers are time-like, i.e. all virtualities
. The maximum allowed virtuality
scale
is set by the hard-scattering process, and
thereafter the virtuality is decreased in each subsequent
branching, down to the cut-off scale
. This cut-off scale
is used to regulate both soft and collinear divergences in the
emission probabilities.
The main points of the PYTHIA showering algorithm are as follows.
- It is a leading-log algorithm, of the improved, coherent kind,
i.e. with angular ordering.
- It can be used for an arbitrary initial pair of partons
or, in fact, for any number between one and seven given entities
(including hadrons and gauge bosons) although only quarks, gluons,
leptons, squarks and gluinos can initiate a shower.
- The pair of showering partons may be given in any frame, but
the evolution is carried out in the c.m. frame of the showering
partons.
- Energy and momentum are conserved exactly at each step of the
showering process.
- If the initial pair comes from the decay of a known resonance,
an additional rejection technique is used in the gluon emission
off a parton of the pair, so as to reproduce the lowest-order
differential 3-jet cross section.
- In subsequent branchings, angular
ordering (coherence effects) is imposed.
- Gluon helicity effects, i.e. correlations between the
production plane and the decay plane of a gluon, can be included.
- The first-order
expression is used, with the
scale given by (an
approximation to) the squared transverse momentum of a branching.
The default
,
which should not be regarded as a proper
, is 0.29 GeV.
- The parton shower is by default
cut off at a mass scale of 1 GeV.
Let us now proceed with a more detailed description.
Subsections
Next: The choice of evolution
Up: Initial- and Final-State Radiation
Previous: Matching to the hard
  Contents
Stephen Mrenna
2004-03-12