monte carlo event generator
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2021 ◽  
Vol 81 (11) ◽  
Author(s):  
S. Jadach ◽  
W. Płaczek ◽  
M. Skrzypek ◽  
B. F. L. Ward

AbstractWe present an estimation of the theoretical precision of low angle Bhabha scattering at the proposed future ILC collider at 500 GeV. The analysis is an extension of the previous analysis done for the FCCee collider at $$\sqrt{s}=M_Z$$ s = M Z . As the state-of-the-art and the reference point we use the Monte Carlo event generator. Based on the current precision status of for LEP analysis, we estimate how various error components evolve from the LEP to ILC setups. The conclusion of our work is that for the ILC the precision of the current version of 4.04 deteriorates to 0.5%, by more than an order of magnitude w.r.t. the present precision for LEP. With the expected future improvements, the precision of can change to 0.016%, nearly as good as for the FCCee at the $$M_Z$$ M Z setup (0.01%). Based on the developed methodology we present also results for ILC$$_{1000}$$ 1000 , FCCee$$_{350}$$ 350 and CLIC$$_{3000}$$ 3000 setups.


2021 ◽  
Vol 5 (1) ◽  
Author(s):  
Andrea Valassi ◽  
◽  
Efe Yazgan ◽  
Josh McFayden ◽  
Simone Amoroso ◽  
...  

AbstractWe review the main software and computing challenges for the Monte Carlo physics event generators used by the LHC experiments, in view of the High-Luminosity LHC (HL-LHC) physics programme. This paper has been prepared by the HEP Software Foundation (HSF) Physics Event Generator Working Group as an input to the LHCC review of HL-LHC computing, which has started in May 2020.


2021 ◽  
Vol 81 (5) ◽  
Author(s):  
S. Baranov ◽  
A. Bermudez Martinez ◽  
L. I. Estevez Banos ◽  
F. Guzman ◽  
F. Hautmann ◽  
...  

AbstractThe Cascade3 Monte Carlo event generator based on Transverse Momentum Dependent (TMD) parton densities is described. Hard processes which are generated in collinear factorization with LO multileg or NLO parton level generators are extended by adding transverse momenta to the initial partons according to TMD densities and applying dedicated TMD parton showers and hadronization. Processes with off-shell kinematics within $$k_{{t}}$$ k t -factorization, either internally implemented or from external packages via LHE files, can be processed for parton showering and hadronization. The initial state parton shower is tied to the TMD parton distribution, with all parameters fixed by the TMD distribution.


2019 ◽  
Vol 79 (12) ◽  
Author(s):  
Johannes Bellm ◽  
Cody B Duncan ◽  
Stefan Gieseke ◽  
Miroslav Myska ◽  
Andrzej Siódmok

AbstractWe present a model for generating spacetime coordinates in the Monte Carlo event generator Herwig 7, and perform colour reconnection by minimizing a boost-invariant distance measure of the system. We compare the model to a series of soft physics observables. We find reasonable agreement with the data, suggesting that pp-collider colour reconnection may be able to be applied in larger systems.


2019 ◽  
Vol 7 (3) ◽  
Author(s):  
Enrico Bothmann ◽  
Gurpreet Singh Chahal ◽  
Stefan Höche ◽  
Johannes Krause ◽  
Frank Krauss ◽  
...  

Sherpa is a general-purpose Monte Carlo event generator for the simulation of particle collisions in high-energy collider experiments. We summarise essential features and improvements of the Sherpa 2.2 release series, which is heavily used for event generation in the analysis and interpretation of LHC Run 1 and Run 2 data. We highlight a decade of developments towards ever higher precision in the simulation of particle-collision events.


2019 ◽  
Vol 218 ◽  
pp. 07004 ◽  
Author(s):  
Carlo M. Carloni Calame ◽  
Guido Montagna ◽  
Oreste Nicrosini ◽  
Fulvio Piccinini

The Monte Carlo event generator BabaYaga has been developed for high precision simulation of QED processes (e+e−→ e+ e− , e+e−→ µ+µ− and e+e−→ γγ) at flavour factories, chiefly for luminometry purposes, with an estimated theoretical accuracy at the 0.1% level or better. QED radiative corrections are included by means of a Parton Shower in QED matched with exact next-to-leading order corrections to reach the required accuracy. The latter is assessed by means of consistent comparisons to independent calculations and an estimate of the size of missing higher-order corrections. The main theoretical framework is overviewed and the status of the generator is summarized.


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