title: ÐÐµÐ½ÐµÑÐ°ÑÐ¾ÑÑ ÑÐ¾Ð±ÑÑÐ¸Ð¹ Ð»ÐµÐ¿ÑÐ¾Ð½-Ð¿ÑÐ¾ÑÐ¾Ð½Ð½Ð¾Ð³Ð¾ Ð²Ð·Ð°Ð¸Ð¼Ð¾Ð´ÐµÐ¹ÑÑÐ²Ð¸Ñ Ð½Ð° Ð¾ÑÐ½Ð¾Ð²Ðµ Ð½ÐµÐ¹ÑÐ¾Ð½Ð½Ð¾Ð¹ ÑÐµÑÐ¸
title: Ð²ÑÐ¿ÑÑÐºÐ½Ð°Ñ ÐºÐ²Ð°Ð»Ð¸ÑÐ¸ÐºÐ°ÑÐ¸Ð¾Ð½Ð½Ð°Ñ ÑÐ°Ð±Ð¾ÑÐ° Ð±Ð°ÐºÐ°Ð»Ð°Ð²ÑÐ°
titleType: Subtitle
title: Event generators of lepton-proton interaction based on a neural network
Creators: name: ÐÐ¾Ð±Ð°Ð½Ð¾Ð², ÐÐ½Ð´ÑÐµÐ¹
Publisher: name: Ð¡Ð°Ð½ÐºÑ-ÐÐµÑÐµÑÐ±ÑÑÐ³ÑÐºÐ¸Ð¹ Ð¿Ð¾Ð»Ð¸ÑÐµÑÐ½Ð¸ÑÐµÑÐºÐ¸Ð¹ ÑÐ½Ð¸Ð²ÐµÑÑÐ¸ÑÐµÑ ÐÐµÑÑÐ° ÐÐµÐ»Ð¸ÐºÐ¾Ð³Ð¾
Year: 2023
Subjects: Ð¼Ð°ÑÐ¸Ð½Ð½Ð¾Ðµ Ð¾Ð±ÑÑÐµÐ½Ð¸Ðµ
Ð³Ð»ÑÐ±Ð¾ÐºÐ¾ Ð½ÐµÑÐ¿ÑÑÐ³Ð¾Ðµ ÑÐ°ÑÑÐµÑÐ½Ð¸Ðµ
Ð³ÐµÐ½ÐµÑÐ°ÑÐ¸Ð²Ð½Ð¾-ÑÐ¾ÑÑÑÐ·Ð°ÑÐµÐ»ÑÐ½ÑÐµ ÑÐµÑÐ¸
machine learning
depp inelastic scattering
generative-adversirial networks

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description: One of the important tasks of modern physics is to study the structure of the proton. A complete theoretical description of the structure of the proton is currently unavaiable. As a result, it is necessary to involve complex feminological models to develop various Monte Carlo event generators. It is well known that deeply inelastic lepton-proton scattering allows one to study the internal structure of the proton. The complementary approach is to use machine learning and neural network techniques, which can produce a model capable of fast and computationally intensive prediction , e.g. the final state of the lepton as a result of deep inelastic lepton-proton scattering. In this work is consider the application of generative-adversarial networks to construct an event generator for deep inelastic lepton-proton scattering at different initial energiesâ and in differentconfigurationsdeepinelasticscattering:inclusive, semi-inclusive, and semi-inclusive with polarization of the incoming proton. In all considered types of deep inelastic scattering, it was obtained that the generative-state network model is capable of predicting the final state of the lepton and hadron both at the initial energies at which the models were trained (20, 40, 60, 80, 100 GeV), and at interpolated (30, 50, 70, 90 GeV), and extrapolated (120, 140, 160, 180 GeV) energies.