In blowout regime of wakefield excitation, strong chaotization of wake occurs. However, for electron-positron colliders and X-ray microscopes, a weakly nonlinear regime is proposed with the formation of a regular short chain of bubbles. To increase the efficiency of the wakefield accelerator, it is necessary that not separate bunches participate. In this paper in 2D plane geometry, the dependence of the number of formed bubbles and their regularization on the degree of wake non-linearity and parameters: driver current, ion mobility, transverse plasma size and profile is studied. We will show that in a weakly nonlinear regime the regular chain of bubbles becomes longer.
在唤醒场激发的井喷状态下,唤醒场会发生强烈的混沌化。然而,对于电子-正电子对撞机和 X 射线显微镜,提出了一种弱非线性机制,即形成规则的短气泡链。为了提高唤醒场加速器的效率,有必要让不独立的气泡串参与其中。本文在二维平面几何中研究了形成气泡的数量及其正则化对唤醒非线性程度和参数的依赖性:驱动电流、离子迁移率、横向等离子体尺寸和剖面 。我们将证明,在弱非线性状态下,规则气泡链会变得更长。
{"title":"REGULARIZATION OF WAKEFIELD IN A WEAKLY NONLINEAR REGIME","authors":"I.V. Demydenko","doi":"10.46813/2023-148-080","DOIUrl":"https://doi.org/10.46813/2023-148-080","url":null,"abstract":"In blowout regime of wakefield excitation, strong chaotization of wake occurs. However, for electron-positron colliders and X-ray microscopes, a weakly nonlinear regime is proposed with the formation of a regular short chain of bubbles. To increase the efficiency of the wakefield accelerator, it is necessary that not separate bunches participate. In this paper in 2D plane geometry, the dependence of the number of formed bubbles and their regularization on the degree of wake non-linearity and parameters: driver current, ion mobility, transverse plasma size and profile is studied. We will show that in a weakly nonlinear regime the regular chain of bubbles becomes longer.","PeriodicalId":54580,"journal":{"name":"Problems of Atomic Science and Technology","volume":"1 1‐2","pages":""},"PeriodicalIF":0.2,"publicationDate":"2023-12-12","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"139009865","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
A. Zykov, N. Yefymenko, S. Dudin, S. Yakovin, N. Azarenkov
The design and characteristics of the combined Magnetron-Ion-Plasma System (MIPS) are presented. The system includes a magnetron sputtering system and a Hall-type ion source with a common magnetic system and common power supply allowing the generation of quasi-neutral ion-electron flow, which provides complete charge neutralization on the processed dielectric surface. The formation of the anode electron layer and the energy spectra of ions are experimentally investigated. A phenomenological model of the combined discharge in EН fields is proposed. Theoretical calculations and experimental data are in reasonable agreement.
{"title":"GENERATION OF COMPENSATED ION-ELECTRON FLOW IN THE COMBINED MAGNETRON-ION-PLASMA SYSTEM","authors":"A. Zykov, N. Yefymenko, S. Dudin, S. Yakovin, N. Azarenkov","doi":"10.46813/2023-148-090","DOIUrl":"https://doi.org/10.46813/2023-148-090","url":null,"abstract":"The design and characteristics of the combined Magnetron-Ion-Plasma System (MIPS) are presented. The system includes a magnetron sputtering system and a Hall-type ion source with a common magnetic system and common power supply allowing the generation of quasi-neutral ion-electron flow, which provides complete charge neutralization on the processed dielectric surface. The formation of the anode electron layer and the energy spectra of ions are experimentally investigated. A phenomenological model of the combined discharge in EН fields is proposed. Theoretical calculations and experimental data are in reasonable agreement.","PeriodicalId":54580,"journal":{"name":"Problems of Atomic Science and Technology","volume":"38 4","pages":""},"PeriodicalIF":0.2,"publicationDate":"2023-12-12","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"139007873","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
2.5D numerical simulation was carried out of the process of ions isolation from electrons of a compensated ion beam by the cusp magnetic field of the before entering the accelerating gap located in the region of zero magnetic field of the cusp, followed by the compensation of the accelerated ion beam with new electrons and transportation of the compensated ion beam to the next section of the linear induction ion accelerator. In contrast to the previously simulated compensated high-current ion beam with an energy of 250 keV (now non-existent), the equivalent plasma flow of a traditional coaxial plasma gun with real parameters: density 1010…1012 cm-3 and velocity 107 cm/s was considered as an injected compensated ion beam.
{"title":"ISOLATION OF ELECTRONS BY THE MAGNETIC FIELD\u0000OF A CUSP FOR HIGH-DENSITY ION BEAM ACCELERATION","authors":"O. V. Fedorovskaya, V. Maslov, I. Onishchenko","doi":"10.46813/2023-148-096","DOIUrl":"https://doi.org/10.46813/2023-148-096","url":null,"abstract":"2.5D numerical simulation was carried out of the process of ions isolation from electrons of a compensated ion beam by the cusp magnetic field of the before entering the accelerating gap located in the region of zero magnetic field of the cusp, followed by the compensation of the accelerated ion beam with new electrons and transportation of\u0000the compensated ion beam to the next section of the linear induction ion accelerator. In contrast to the previously simulated compensated high-current ion beam with an energy of 250 keV (now non-existent), the equivalent plasma flow of a traditional coaxial plasma gun with real parameters: density 1010…1012 cm-3 and velocity 107 cm/s was\u0000considered as an injected compensated ion beam.","PeriodicalId":54580,"journal":{"name":"Problems of Atomic Science and Technology","volume":"49 151","pages":""},"PeriodicalIF":0.2,"publicationDate":"2023-12-12","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"139007964","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}