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Precision Monte Carlo simulations with WHIZARD

The precision physics programs of FCC-ee demands for a precise simulation of all Standard Model (SM) processes and possible beyond the SM (BSM) signals in a state-of-the-art way by means of Monte Carlo (MC) techniques. As a standard tool for e +e − simulations, the multipurpose event generator WHIZA...

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Detalles Bibliográficos
Autores principales: Braß, S, Kilian, W, Ohl, T, Reuter, J, Rothe, V, Stienemeier, P
Lenguaje:eng
Publicado: 2019
Materias:
Acceso en línea:https://dx.doi.org/10.23731/CYRM-2020-003.205
http://cds.cern.ch/record/2701767
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author Braß, S
Kilian, W
Ohl, T
Reuter, J
Rothe, V
Stienemeier, P
author_facet Braß, S
Kilian, W
Ohl, T
Reuter, J
Rothe, V
Stienemeier, P
author_sort Braß, S
collection CERN
description The precision physics programs of FCC-ee demands for a precise simulation of all Standard Model (SM) processes and possible beyond the SM (BSM) signals in a state-of-the-art way by means of Monte Carlo (MC) techniques. As a standard tool for e +e − simulations, the multipurpose event generator WHIZARD [1, 2] has been used: this generator has been originally developed for the TESLA project, and later on been used e.g. for the ILC Technical Design Report [3,4]. The WHIZARD package has a modular structure which serves a modern unit-test driven software development and guarantees a high level of maintainability and extendability. WHIZARD comes with its own fully general tree-level matrix-element generator for the hard process, O’Mega [5]. It generates amplitudes in a recursive way based on the graph-theoretical concepts of directed acyclical graphs (DAGs), thereby avoiding all redundancies. The matrix elements are generated either as compilable modern Fortran code or as bytecode instructions interpreted by a virtual machine [6]. For QCD, WHIZARD uses the color-flow formalism [7]. Matrix elements support all kinds of particles and interactions up to spin-2. A large number of BSM models is hard-coded, particularly the MSSM and NMSSM [8, 9]. General BSM models can be loaded from a Lagrangian level tool, using the interface to FeynRules [10]; from the version 2.8.0 of WHIZARD on (early summer 2019) a full-fledged interface to the general UFO format will be available. One of the biggest assets of WHIZARD is its general phasespace parameterization which uses a heuristic based on the dominating sub-processes, which allows to integrate and simulate processes with up to 10 fermions in the final state. The integration is based on an adaptive multi-channel algorithm, called VAMP [11]. Recently, this multi-channel adaptive integration has been enhanced to a parallelized version using the MPI3 protocol showing speedups of up to 100 [12], while a first physics study using this MPI parallelized integration and event generation has been published in [13].
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institution Organización Europea para la Investigación Nuclear
language eng
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spelling oai-inspirehep.net-17373872020-10-16T22:19:00Zdoi:10.23731/CYRM-2020-003.205http://cds.cern.ch/record/2701767engBraß, SKilian, WOhl, TReuter, JRothe, VStienemeier, PPrecision Monte Carlo simulations with WHIZARDParticle Physics - PhenomenologyThe precision physics programs of FCC-ee demands for a precise simulation of all Standard Model (SM) processes and possible beyond the SM (BSM) signals in a state-of-the-art way by means of Monte Carlo (MC) techniques. As a standard tool for e +e − simulations, the multipurpose event generator WHIZARD [1, 2] has been used: this generator has been originally developed for the TESLA project, and later on been used e.g. for the ILC Technical Design Report [3,4]. The WHIZARD package has a modular structure which serves a modern unit-test driven software development and guarantees a high level of maintainability and extendability. WHIZARD comes with its own fully general tree-level matrix-element generator for the hard process, O’Mega [5]. It generates amplitudes in a recursive way based on the graph-theoretical concepts of directed acyclical graphs (DAGs), thereby avoiding all redundancies. The matrix elements are generated either as compilable modern Fortran code or as bytecode instructions interpreted by a virtual machine [6]. For QCD, WHIZARD uses the color-flow formalism [7]. Matrix elements support all kinds of particles and interactions up to spin-2. A large number of BSM models is hard-coded, particularly the MSSM and NMSSM [8, 9]. General BSM models can be loaded from a Lagrangian level tool, using the interface to FeynRules [10]; from the version 2.8.0 of WHIZARD on (early summer 2019) a full-fledged interface to the general UFO format will be available. One of the biggest assets of WHIZARD is its general phasespace parameterization which uses a heuristic based on the dominating sub-processes, which allows to integrate and simulate processes with up to 10 fermions in the final state. The integration is based on an adaptive multi-channel algorithm, called VAMP [11]. Recently, this multi-channel adaptive integration has been enhanced to a parallelized version using the MPI3 protocol showing speedups of up to 100 [12], while a first physics study using this MPI parallelized integration and event generation has been published in [13].oai:inspirehep.net:17373872019
spellingShingle Particle Physics - Phenomenology
Braß, S
Kilian, W
Ohl, T
Reuter, J
Rothe, V
Stienemeier, P
Precision Monte Carlo simulations with WHIZARD
title Precision Monte Carlo simulations with WHIZARD
title_full Precision Monte Carlo simulations with WHIZARD
title_fullStr Precision Monte Carlo simulations with WHIZARD
title_full_unstemmed Precision Monte Carlo simulations with WHIZARD
title_short Precision Monte Carlo simulations with WHIZARD
title_sort precision monte carlo simulations with whizard
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.23731/CYRM-2020-003.205
http://cds.cern.ch/record/2701767
work_keys_str_mv AT braßs precisionmontecarlosimulationswithwhizard
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AT ohlt precisionmontecarlosimulationswithwhizard
AT reuterj precisionmontecarlosimulationswithwhizard
AT rothev precisionmontecarlosimulationswithwhizard
AT stienemeierp precisionmontecarlosimulationswithwhizard