23 research outputs found

    Fast simulation of muons produced at the SHiP experiment using generative adversarial networks

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    This paper presents a fast approach to simulating muons produced in interactions of the SPS proton beams with the target of the SHiP experiment. The SHiP experiment will be able to search for new long-lived particles produced in a 400 GeV/c SPS proton beam dump and which travel distances between fifty metres and tens of kilometers. The SHiP detector needs to operate under ultra-low background conditions and requires large simulated samples of muon induced background processes. Through the use of Generative Adversarial Networks it is possible to emulate the simulation of the interaction of 400 GeV/c proton beams with the SHiP target, an otherwise computationally intensive process. For the simulation requirements of the SHiP experiment, generative networks are capable of approximating the full simulation of the dense fixed target, offering a speed increase by a factor of Script O(106). To evaluate the performance of such an approach, comparisons of the distributions of reconstructed muon momenta in SHiP's spectrometer between samples using the full simulation and samples produced through generative models are presented. The methods discussed in this paper can be generalised and applied to modelling any non-discrete multi-dimensional distribution

    The experimental facility for the Search for Hidden Particles at the CERN SPS

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    The International School for Advanced Studies (SISSA) logo The International School for Advanced Studies (SISSA) logo The following article is OPEN ACCESS The experimental facility for the Search for Hidden Particles at the CERN SPS C. Ahdida44, R. Albanese14,a, A. Alexandrov14, A. Anokhina39, S. Aoki18, G. Arduini44, E. Atkin38, N. Azorskiy29, J.J. Back54, A. Bagulya32Show full author list Published 25 March 2019 ‱ © 2019 CERN Journal of Instrumentation, Volume 14, March 2019 Download Article PDF References Download PDF 543 Total downloads 7 7 total citations on Dimensions. Article has an altmetric score of 1 Turn on MathJax Share this article Share this content via email Share on Facebook Share on Twitter Share on Google+ Share on Mendeley Article information Abstract The Search for Hidden Particles (SHiP) Collaboration has shown that the CERN SPS accelerator with its 400 GeV/c proton beam offers a unique opportunity to explore the Hidden Sector [1–3]. The proposed experiment is an intensity frontier experiment which is capable of searching for hidden particles through both visible decays and through scattering signatures from recoil of electrons or nuclei. The high-intensity experimental facility developed by the SHiP Collaboration is based on a number of key features and developments which provide the possibility of probing a large part of the parameter space for a wide range of models with light long-lived super-weakly interacting particles with masses up to Script O(10) GeV/c2 in an environment of extremely clean background conditions. This paper describes the proposal for the experimental facility together with the most important feasibility studies. The paper focuses on the challenging new ideas behind the beam extraction and beam delivery, the proton beam dump, and the suppression of beam-induced background

    CIVIL-LAW RELATIONS CONNECTED WITHN USING OF THE ELECTRONIC SIGNATURE

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    В ŃŃ‚Đ°Ń‚ŃŒĐ” ĐžŃŃĐ»Đ”ĐŽŃƒĐ”Ń‚ŃŃ ĐžŃĐżĐŸĐ»ŃŒĐ·ĐŸĐČĐ°ĐœĐžĐ” ŃĐ»Đ”ĐșŃ‚Ń€ĐŸĐœĐœĐŸĐč ĐżĐŸĐŽĐżĐžŃĐž ĐČ ĐłŃ€Đ°Đ¶ĐŽĐ°ĐœŃĐșĐŸ-праĐČĐŸĐČых ĐŸŃ‚ĐœĐŸŃˆĐ”ĐœĐžŃŃ…, Đ° таĐșжД ĐłŃ€Đ°Đ¶ĐŽĐ°ĐœŃĐșĐŸ-праĐČĐŸĐČŃ‹Đ” ĐŸŃ‚ĐœĐŸŃˆĐ”ĐœĐžŃ ĐżĐŸ ДД ĐżĐŸĐ»ŃƒŃ‡Đ”ĐœĐžŃŽ. ĐĄĐŽĐ”Đ»Đ°ĐœŃ‹ ĐČыĐČĐŸĐŽŃ‹ ĐŸ Ń‚ĐŸĐŒ, Ń‡Ń‚ĐŸ ŃĐ»Đ”ĐșŃ‚Ń€ĐŸĐœĐœĐ°Ń ĐżĐŸĐŽĐżĐžŃŃŒ ĐŒĐŸĐ¶Đ”Ń‚ ĐžŃĐżĐŸĐ»ŃŒĐ·ĐŸĐČаться ĐČ Ń€Đ°Đ·ĐœŃ‹Ń… ĐČоЮах ĐłŃ€Đ°Đ¶ĐŽĐ°ĐœŃĐșох праĐČĐŸĐŸŃ‚ĐœĐŸŃˆĐ”ĐœĐžĐč. ĐŸĐ”Ń€ŃĐżĐ”ĐșтоĐČĐœŃ‹ĐŒĐž ĐŽĐ»Ń Ń€Đ°ŃŃˆĐžŃ€Đ”ĐœĐžŃ ДД ĐžŃĐżĐŸĐ»ŃŒĐ·ĐŸĐČĐ°ĐœĐžŃ яĐČĐ»ŃŃŽŃ‚ŃŃ ĐŽĐŸĐłĐŸĐČĐŸŃ€ĐœŃ‹Đ”, ĐČĐ”Ń‰ĐœŃ‹Đ” Đž ĐșĐŸŃ€ĐżĐŸŃ€Đ°Ń‚ĐžĐČĐœŃ‹Đ” ĐŸŃ‚ĐœĐŸŃˆĐ”ĐœĐžŃ. ĐžŃ‚ĐœĐŸŃˆĐ”ĐœĐžŃ ĐżĐŸ ĐżĐŸĐČĐŸĐŽŃƒ ДД ĐżĐŸĐ»ŃƒŃ‡Đ”ĐœĐžŃ ĐČ ŃƒĐŽĐŸŃŃ‚ĐŸĐČĐ”Ń€ŃŃŽŃ‰Đ”ĐŒ Ń†Đ”ĐœŃ‚Ń€Đ” ĐŸĐżĐŸŃŃ€Đ”ĐŽŃƒŃŽŃ‚ŃŃ ĐŽĐŸĐłĐŸĐČĐŸŃ€ĐŸĐŒ ĐŸĐșĐ°Đ·Đ°ĐœĐžŃ услуг. ВыяĐČĐ»Đ”ĐœŃ‹ праĐșтОчДсĐșОД сотуацоо, сĐČĐžĐŽĐ”Ń‚Đ”Đ»ŃŒŃŃ‚ĐČŃƒŃŽŃ‰ĐžĐ” ĐŸ ĐœĐ”ĐŽĐŸŃŃ‚Đ°Ń‚Đșах ĐżŃ€ĐŸŃ†Đ”ĐŽŃƒŃ€Ń‹ ĐżĐŸĐ»ŃƒŃ‡Đ”ĐœĐžŃ Đž ĐžŃĐżĐŸĐ»ŃŒĐ·ĐŸĐČĐ°ĐœĐžŃ ŃĐ»Đ”ĐșŃ‚Ń€ĐŸĐœĐœĐŸĐč ĐżĐŸĐŽĐżĐžŃĐž. Đ˜ŃŃĐ»Đ”ĐŽĐŸĐČĐ°ĐœŃ‹ ĐžĐ·ĐŒĐ”ĐœĐ”ĐœĐžŃ Đ·Đ°ĐșĐŸĐœĐŸĐŽĐ°Ń‚Đ”Đ»ŃŒŃŃ‚ĐČĐ°, ĐșĐŸŃ‚ĐŸŃ€Ń‹Đ” ŃƒĐ¶Đ”ŃŃ‚ĐŸŃ‡Đ°ŃŽŃ‚ Ń‚Ń€Đ”Đ±ĐŸĐČĐ°ĐœĐžŃ Đș ŃƒĐŽĐŸŃŃ‚ĐŸĐČĐ”Ń€ŃŃŽŃ‰ĐžĐŒ Ń†Đ”ĐœŃ‚Ń€Đ°ĐŒ Đž ŃĐŸĐČĐ”Ń€ŃˆĐ”ĐœŃŃ‚ĐČуют ĐżŃ€ĐŸŃ†Đ”ĐŽŃƒŃ€Ńƒ ĐżĐŸĐ»ŃƒŃ‡Đ”ĐœĐžŃ ŃĐ»Đ”ĐșŃ‚Ń€ĐŸĐœĐœĐŸĐč ĐżĐŸĐŽĐżĐžŃĐž ĐČ Ń†Đ”Đ»ŃŃ… ŃƒŃŃ‚Ń€Đ°ĐœĐ”ĐœĐžŃ Đ·Đ»ĐŸŃƒĐżĐŸŃ‚Ń€Đ”Đ±Đ»Đ”ĐœĐžĐč ĐżĐŸ ДД ĐžŃĐżĐŸĐ»ŃŒĐ·ĐŸĐČĐ°ĐœĐžŃŽ.The article examines using of an electronic signature in various types of civil law relations and civil law relations on receiving of an electronic signature. Conclusions are drawn that the electronic signature can be used in various types of civil law relations. Contractual, property and corporate relations are promising for the development of its use. Relations on receiving of the electronic signature in the certification center are mediated by a service agreement. Practical situations have been identified that testify to the shortcomings of the procedure for obtaining and using the electronic signature. Legislative changes are studied that tighten the requirements for certification centers and improve the procedure for obtaining the electronic signature to eliminate abuses in its use

    Biopsychosocial approach in the rehabilitation of patients with operable breast cancer

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    The relevance: more than 60% of cases are due to early breast cancer (EBC). Priority is the treatment of patients with early breast cancer, provided that the maximum quality of life (QL) is maintained. During or after complex treatment, more than half of patients with EBC report the occurrence of functional disorders that reduce the QL. Aim: to evaluate the event-free survival rate (EFS) of EBC patients undergoing rehabilitation within the framework of a biopsychosocial approach in the course of complex antitumor treatment. Materials and methods: the study involved 228 patients with EBC who received complex treatment from 2015 to 2019. In the prospective part of the study, 114 patients were subjected to rehabilitation measures in the framework of a biopsychosocial approach that considers both biological features of functional restriction and psychosocial disorders, a multidisciplinary team of specialists worked with all patients. In the control group, 114 patients were selected retrospectively and underwent physical and psychological rehabilitation as prescribed by a doctor. Patients of both groups are divided into subgroups depending on the availability of preoperative chemotherapy. Event-free survival was assessed over a 2-year follow-up period. Events were accepted as censored events: relapse, metastases, the occurrence of another cancer, a new concomitant disease, an exacerbation of concomitant pathology, and death. Results: Rehabilitation measures within the framework of the biopsychosocial model improve the indicators of EFS in patients with EBC. The use of a biopsychosocial approach in rehabilitation increased EFS by 3.8 months. The results of multivariate analysis, reducing the risk of occurrence of the event EBC patients undergoing rehabilitation within the framework of the biopsychosocial approach in the presence of neoadjuvant chemotherapy was 28%, in patients of younger age group (25–44 years) was 29%, in patients in menopause – 25%

    SHiP Experiment-Comprehensive Design Study report

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    Fast simulation of muons produced at the SHiP experiment using Generative Adversarial Networks

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    This paper presents a fast approach to simulating muons produced in interactions of the SPS proton beams with the target of the SHiP experiment. The SHiP experiment will be able to search for new long-lived particles produced in a 400 GeV/c SPS proton beam dump and which travel distances between fifty metres and tens of kilometers. The SHiP detector needs to operate under ultra-low background conditions and requires large simulated samples of muon induced background processes. Through the use of Generative Adversarial Networks it is possible to emulate the simulation of the interaction of 400 GeV/c proton beams with the SHiP target, an otherwise computationally intensive process. For the simulation requirements of the SHiP experiment, generative networks are capable of approximating the full simulation of the dense fixed target, offering a speed increase by a factor of (106). To evaluate the performance of such an approach, comparisons of the distributions of reconstructed muon momenta in SHiP's spectrometer between samples using the full simulation and samples produced through generative models are presented. The methods discussed in this paper can be generalised and applied to modelling any non-discrete multi-dimensional distribution

    Fast simulation of muons produced at the SHiP experiment using Generative Adversarial Networks

    Get PDF
    This paper presents a fast approach to simulating muons produced in interactions of the SPS proton beams with the target of the SHiP experiment. The SHIP experiment will be able to search for new long-lived particles produced in a 400 GeV/c SPS proton beam dump and which travel distances between fifty metres and tens of kilometers. The SHiP detector needs to operate under ultra-low background conditions and requires large simulated samples of muon induced background processes. Through the use of Generative Adversarial Networks it is possible to emulate the simulation of the interaction of 400 GeV/c proton beams with the SHiP target, an otherwise computationally intensive process. For the simulation requirements of the SHiP experiment, generative networks are capable of approximating the full simulation of the dense fixed target, offering a speed increase by a factor of O(10(6)). To evaluate the performance of such an approach, comparisons of the distributions of reconstructed muon momenta in SHiP's spectrometer between samples using the full simulation and samples produced through generative models are presented. The methods discussed in this paper can be generalised and applied to modelling any non-discrete multi-dimensional distribution

    The magnet of the scattering and neutrino detector for the SHiP experiment at CERN

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    The Search for Hidden Particles (SHiP) experiment proposal at CERN demands a dedicated dipole magnet for its scattering and neutrino detector. This requires a very large volume to be uniformly magnetized at B > 1.2 T, with constraints regarding the inner instrumented volume as well as the external region, where no massive structures are allowed and only an extremely low stray field is admitted. In this paper we report the main technical challenges and the relevant design options providing a comprehensive design for the magnet of the SHiP Scattering and Neutrino Detector

    The Magnet of the Scattering and Neutrino Detector for the SHiP experiment at CERN

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    The Search for Hidden Particles (SHiP) experiment proposal at CERN demands a dedicated dipole magnet for its scattering and neutrino detector. This requires a very large volume to be uniformly magnetized at B>1.2 T, with constraints regarding the inner instrumented volume as well as the external region, where no massive structures are allowed and only an extremely low stray field is admitted. In this paper we report the main technical challenges and the relevant design options providing a comprehensive design for the magnet of the SHiP Scattering and Neutrino Detector.The Search for Hidden Particles (SHiP) experiment proposal at CERN demands a dedicated dipole magnet for its scattering and neutrino detector. This requires a very large volume to be uniformly magnetized at B > 1.2 T, with constraints regarding the inner instrumented volume as well as the external region, where no massive structures are allowed and only an extremely low stray field is admitted. In this paper we report the main technical challenges and the relevant design options providing a comprehensive design for the magnet of the SHiP Scattering and Neutrino Detector
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