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PYTHIA 6.4 Physics and Manual

PYTHIA 6.4 Physics and Manual

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WDTPM, WDTEM, XLAM <strong>and</strong> IDLAM, have been exp<strong>and</strong>ed from dimension 300 to 400.• Lepton- <strong>and</strong> baryon-number-violating decay channels have been included for supersymmetricparticles [Ska01, Sjö03]. Thus the decay tables have grown considerablylonger.• The string hadronization scheme has been improved <strong>and</strong> exp<strong>and</strong>ed better to h<strong>and</strong>lejunction topologies, where three strings meet. This is relevant for baryon-numberviolatingprocesses, <strong>and</strong> also for the h<strong>and</strong>ling of baryon beam remnants. Thus newroutines have been introduced, <strong>and</strong> also e.g. new K(I,1) status codes.• A runtime interface to Isasusy has been added, for determining the SUSY massspectrum <strong>and</strong> mixing parameters more accurately than with the internal Pythiaroutines.• The Technicolor scenario is updated <strong>and</strong> extended. A new common block, PYTCSM,is introduced for the parameters <strong>and</strong> switches in Technicolor <strong>and</strong> related scenarios,<strong>and</strong> variables are moved to it from a few other common blocks. New processes381–388 are introduced for st<strong>and</strong>ard QCD 2 → 2 interactions with Technicolor (orother compositeness) extensions, while the processes 11, 12, 13, 28, 53, 68, 81 <strong>and</strong>82 now revert back to being pure QCD.• The PYSHOW time-like showering routine has been exp<strong>and</strong>ed to allow showering insidesystems consisting of up to 80 particles, which can be made use of in some resonancedecays <strong>and</strong> in user-defined processes.• The PYSSPA space-like showering routine has been exp<strong>and</strong>ed with a q → qγ branching.• The PYSIGH routine has been split into several, in order to make it more manageable.(It had increased to a size of over 7000 lines, which gave some compilersproblems.) All the phase-space <strong>and</strong> parton-density generic weights remain, whereasthe process-specific matrix elements have been grouped into new routines PYSGQC,PYSGHF, PYSGWZ, PYSGHG, PYSGSU, PYSGTC <strong>and</strong> PYSGEX.• Some exotic particles <strong>and</strong> QCD effective states have been moved from temporaryflavour codes to a PDG-consistent naming, <strong>and</strong> a few new codes have been introduced.• The maximum number of documentation lines in the beginning of the event recordhas been exp<strong>and</strong>ed from 50 to 100.• The default parton distribution set for the proton is now CTEQ 5L.• The default St<strong>and</strong>ard Model Higgs mass has been changed to 115 GeV.Changes in version 6.3: The major changes in 6.3 was the introduction of a newunderlying–event framework for hadron collisions, together with new transverse-momentum-orderedinitial- <strong>and</strong> final-state parton showers. Other changes include an interfaceto SUSY spectrum <strong>and</strong> decay calculators conformant to the SUSY Les Houches Accord.Early releases of Pythia 6.3, up to 6.312, were still experimental, <strong>and</strong> did not include thenew parton showers. Details on these versions can be found in the update notes availableon the web. We here concentrate on the structure of the program after (<strong>and</strong> including)version 6.312.Firstly, there are no incompatibilities between Pythia 6.2 <strong>and</strong> Pythia 6.3 at thelevel of commonblock sizes or subroutine arguments (except for the PYSUGI interface toIsajet, see below). That is, any program that ran with Pythia 6.2 also ought to runwith Pythia 6.3, without any change required. Note, however, the following news:• The old (6.2) master event-generation routine PYEVNT is still available; it uses the oldunderlying–event machinery (PYMULT) <strong>and</strong> parton showers (PYSSPA <strong>and</strong> PYSHOW). A‘Tune A’–like set of parameters [Fie02] has been adopted as default. It reproducesTune A at the Tevatron, but implies a slower energy rescaling, to give a moreconservative estimate of the underlying activity at the LHC.26

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