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pegasus:overview [15/04/2024 10:09] – lipatovpegasus:overview [15/04/2024 10:13] – lipatov
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 The calculations using PEGASUS include a few general steps common for all of the processes. The calculations using PEGASUS include a few general steps common for all of the processes.
-When PEGASUS is running, one can select the colliding particles, proton-proton, proton-antiproton or electron-proton,  +When PEGASUS is running, one can select the colliding particles, proton-proton, proton-antiproton, proton-nucleus or electron-proton,  
-and set their center-of-mass energy. The default setting corresponds to the LHC Run II setup.+and set beam energies. The default setting corresponds to the LHC Run II setup.
 Then one can select factorization scheme (TMD or collinear one) for each of the colliding particles, choose corresponding parton density function and set the parameters, important  Then one can select factorization scheme (TMD or collinear one) for each of the colliding particles, choose corresponding parton density function and set the parameters, important 
 for further Monte-Carlo simulation, namely, number of iterations and number of simulated events per iteration. for further Monte-Carlo simulation, namely, number of iterations and number of simulated events per iteration.
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 ^ Set      ^  Order of a<sub>s</sub>      ^  N<sub>f</sub>  ^  QCD scale [MeV]  ^  Reference  ^ ^ Set      ^  Order of a<sub>s</sub>      ^  N<sub>f</sub>  ^  QCD scale [MeV]  ^  Reference  ^
-| LLM'2022 (CCFM)  |  2  |  4  |  200  |  [[https://arxiv.org/abs/2211.03727|A.V. Lipatov, G.I. Lykasov, M.A. Malyshev]]  |+| LLM (CCFM)  |  2  |  4  |  200  |  [[https://arxiv.org/abs/2211.03727|A.V. Lipatov, G.I. Lykasov, M.A. Malyshev]]  |
 | A0 (CCFM)  |  1  |  4  |  250  |  [[https://arxiv.org/abs/hep-ph/0411287|H. Jung]]  | | A0 (CCFM)  |  1  |  4  |  250  |  [[https://arxiv.org/abs/hep-ph/0411287|H. Jung]]  |
 | B0 (CCFM)  |  1  |  4  |  250  |  [[https://arxiv.org/abs/hep-ph/0411287|H. Jung]]  | | B0 (CCFM)  |  1  |  4  |  250  |  [[https://arxiv.org/abs/hep-ph/0411287|H. Jung]]  |
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 with respect to the number of active flavors and QCD scale. with respect to the number of active flavors and QCD scale.
 This choice is done automatically with the choice of the TMD and/or conventional This choice is done automatically with the choice of the TMD and/or conventional
-parton densities in a proton. There is no possibility to change it manually since this setup is essential for determination of corresponding parton distributions.+parton densities. There is no possibility to change it manually since this setup is essential for determination of corresponding parton distributions.
  
 The masses of all particles (quarks, gauge bosons, heavy quarkonia etc), The masses of all particles (quarks, gauge bosons, heavy quarkonia etc),
pegasus/overview.txt · Last modified: 15/04/2024 10:14 by lipatov