کد مقاله کد نشریه سال انتشار مقاله انگلیسی نسخه تمام متن
502982 863734 2008 16 صفحه PDF دانلود رایگان
عنوان انگلیسی مقاله ISI
A brief introduction to PYTHIA 8.1
موضوعات مرتبط
مهندسی و علوم پایه شیمی شیمی تئوریک و عملی
پیش نمایش صفحه اول مقاله
A brief introduction to PYTHIA 8.1
چکیده انگلیسی

The Pythia program is a standard tool for the generation of high-energy collisions, comprising a coherent set of physics models for the evolution from a few-body hard process to a complex multihadronic final state. It contains a library of hard processes and models for initial- and final-state parton showers, multiple parton-parton interactions, beam remnants, string fragmentation and particle decays. It also has a set of utilities and interfaces to external programs. While previous versions were written in Fortran, Pythia 8 represents a complete rewrite in C++. The current release is the first main one after this transition, and does not yet in every respect replace the old code. It does contain some new physics aspects, on the other hand, that should make it an attractive option especially for LHC physics studies.Program summaryProgram title:Pythia 8.1Catalogue identifier: ACTU_v3_0Program summary URL:http://cpc.cs.qub.ac.uk/summaries/ACTU_v3_0.htmlProgram obtainable from: CPC Program Library, Queen's University, Belfast, N. IrelandLicensing provisions: GPL version 2No. of lines in distributed program, including test data, etc.: 176 981No. of bytes in distributed program, including test data, etc.: 2 411 876Distribution format: tar.gzProgramming language: C++Computer: Commodity PCsOperating system: Linux; should also work on other systemsRAM: 8 megabytesClassification: 11.2Does the new version supersede the previous version?: yes, partlyNature of problem: High-energy collisions between elementary particles normally give rise to complex final states, with large multiplicities of hadrons, leptons, photons and neutrinos. The relation between these final states and the underlying physics description is not a simple one, for two main reasons. Firstly, we do not even in principle have a complete understanding of the physics. Secondly, any analytical approach is made intractable by the large multiplicities.Solution method: Complete events are generated by Monte Carlo methods. The complexity is mastered by a subdivision of the full problem into a set of simpler separate tasks. All main aspects of the events are simulated, such as hard-process selection, initial- and final-state radiation, beam remnants, fragmentation, decays, and so on. Therefore events should be directly comparable with experimentally observable ones. The programs can be used to extract physics from comparisons with existing data, or to study physics at future experiments.Reasons for new version: Improved and expanded physics models, transition from Fortran to C++.Summary of revisions: New user interface, transverse-momentum-ordered showers, interleaving with multiple interactions, and much more.Restrictions: Depends on the problem studied.Running time: 10–1000 events per second, depending on process studied.References: [1] T. Sjöstrand, P. Edén, C. Friberg, L. Lönnblad, G. Miu, S. Mrenna, E. Norrbin, Comput. Phys. Comm. 135 (2001) 238.

ناشر
Database: Elsevier - ScienceDirect (ساینس دایرکت)
Journal: Computer Physics Communications - Volume 178, Issue 11, 1 June 2008, Pages 852–867
نویسندگان
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