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Despite the simple structure of the tree-level Perturbative Quantum Field Theory description of the Collision and Decay processes in an event, the observed high-energy process usually contains significant amount of modifications, like Photon and Gluon '' Bremsstrahlung '' or loop Diagram corrections, that usually are too complex to be easily evaluated in real calculations directly on the diagrammatic level. Furthermore, the non-perturbative nature of QCD Bound State s makes it necessary to include information that are outside the perturbative quantum field theory, and well beyond present ability of computation in Lattice QCD . And in collisional systems more complex than a few Lepton s and Hadron s (e.g. heavy-ion collisions), the collective behavior of the system would involve a Phenomenological description that also cannot be easily obtained from the fundamental field theory by a simple calculus.

Any realistic test of the underlying physical process in a Particle Accelerator Experiment , therefore, requires an adequate inclusion of these complex behaviors surrounding the actual process. Based on the fact that in most processes, a Factorization of the full process into individual problems is possible (which means a negligible effect from Interference ), these individual processes are calculated separately, and the Probabilistic branching between them are performed using Monte Carlo Method s.

The final-state particles generated by event generators can be feeded into the detector simulation, allowing a precise prediction and verification for the entire system of experimental setup. However, as the detector simulation is usually a complex and computationally expensive task, simple event analysis techniques are also performed directly on event generator results.

A typical hadronic event generator simulates the following subprocesses:

  • Initial-state composition and substructure

  • Initial-state Shower s

  • The hard process

  • Resonance decay

  • Final-state showers

  • Accompaning semi-hard processes

  • Hadronization and further decay


A typical heavy-ion event generator usually can be less strict in simulating the rare and rather negligible processes found in a hadronic generator, but would need to simulate the following subprocesses, in addition to those in a hadronic generator:

  • Nuclear initial-state

  • High multiplicity, soft processes

  • In-medium energy loss

  • Collective behavior of the medium ''(not handled properly by any generators sofar)''


Partly due to historic reasons, most event generators are written in FORTRAN 77 , with a few C++ generators slowly emerging in recent years. The Particle Data Group maintains a Standard for designating Standard Model particles and Resonances with Integer Code s in event generators (also known as the "PDG code").


LIST OF EVENT GENERATORS

The major event generators that are used by current experiments are:

Hadronic event generators

Heavy ion event generators

Specialized event generators
  • AcerMCLHC background processes

  • ALPGEN – multiple Parton processes

  • Ariadne – QCD cascade with Color Dipole Model

  • MC@NLO – parton shower with next-to-leading-order QCD matrix elements

  • JIMMY – multiple parton processes


"Meta-generator"
  • CompHEP – automatic evaluation of tree level matrix elements for event generation or export into other event generators



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