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A method of generating pulse flows of high-energy particles and particles sources for the implementation of this method

机译:一种产生高能粒子和粒子源的脉冲流的方法,以实现该方法

摘要

1. A method of generating a pulsed flux of energetic particles, comprising the steps of;ion plasma initiation on the first electrode (111) in a vacuum chamber (110) and allowing the development of said plasma toward the second electrode (112) in said vacuum chamber,;supply of a short pulse of high voltage between the electrodes in the time interval during which said ion plasma is in a transitional state with a space distribution of ions or electrons at a distance from said second electrode, so as to accelerate said distributed ions or electrons towards said second electrode , whereby is generated a high-energy flux of charged particles at the same time overcome the current limit associated with the space charge, the conventional vacuum diode, and;generating said energetic particles at said second electrode (112).;2. The method of claim 1, wherein said high energy particles generated by the nuclear or electromagnetic reaction "beam / target" occurring between said accelerated ions or electrons and said second electrode. (112).;3. The method of claim 1, wherein said second electrode is a semi-transparent grid structure, and said high-energy particles are plasma ions or electrons passing through said second electrode (112).;4. A method according to any one of claims 1-3, wherein said predetermined time determined based on at least the voltage level of the pulse, the geometry of the electrodes (111, 112) and the distance between them, and the pressure in the chamber.;5. The method according to any one of claims 1-3, wherein said first electrode (111) comprises a pair of electrode members forming a plasma discharge ion source.;6. The source of high energy particles, comprising;a vacuum chamber (110) comprising a first electrode (111) and a second electrode (112), said first electrode forming a plasma ion source which is able to generate ion plasma and provide plasma ion develop in said chamber towards said second electrode,;a triggering device (131) of the ion source connected to said first electrode for supplying power to a plasma ion source,;a high voltage generator (132) coupled to said first and second electrodes, and;a block (140) of the control and monitoring to ensure the supply of high voltage short pulse between said first and second electrodes in response to excitation of said plasma ion source, said triggering device of the ion source in the time interval during which said ion plasma is in a transitional state with a space distribution ions or electrons at a distance from said second electrode, so as to accelerate said distributed ions or electrons towards said second electrode and generate a high-energy flux of charged particles to overcoming the current limit associated with the space charge, the conventional vacuum diode.;7. The source according to claim 6, wherein said high energy particles generated by the nuclear or electromagnetic reaction "beam / target" occurring between said accelerated ions or electrons and said second electrode (112).;8. The source according to claim 6, wherein said second electrode (112) is a semi-transparent grid structure, and said high-energy particles are plasma ions or electrons directly passing through said second electrode.;9. The source according to claim 6, wherein said block (140) the management and control operable to start said high voltage pulse after a predetermined time delay with respect to the ion plasma generation.;10. The source of claim 9, wherein said time delay is determined based, at least from the level of the voltage pulse, the geometry of the electrodes and distance between them, and the pressure in the chamber.;11. A source according to any one pp.6-10, wherein said first electrode (111) comprises a pair of electrode members forming a plasma discharge ion source.
机译:1。一种产生高能粒子的脉冲通量的方法,包括以下步骤:在真空室(110)中的第一电极(111)上进行离子等离子体引发,并使所述等离子体朝着第二电极(112)发展。所述真空室;在所述离子等离子体处于过渡状态的时间间隔内,在距所述第二电极一定距离的位置具有离子或电子的空间分布的电极之间的短脉冲高电压的供给。朝向所述第二电极的所述分布的离子或电子,从而同时产生高能通量的带电粒子,克服了与空间电荷,常规真空二极管相关的电流限制,并且;在所述第二电极处产生了所述高能粒子(112).; 2。 2.根据权利要求1所述的方法,其中,由核或电磁反应“束/靶”产生的所述高能粒子发生在所述加速离子或电子与所述第二电极之间。 (112).; 3。 2.根据权利要求1所述的方法,其中,所述第二电极是半透明的栅格结构,并且所述高能粒子是穿过所述第二电极(112)的等离子体离子或电子。 4.根据权利要求1-3中任一项所述的方法,其中,所述预定时间至少基于脉冲的电压电平,电极(111、112)的几何形状以及它们之间的距离以及腔室内的压力来确定。 。; 5。 4.根据权利要求1-3中的任一项所述的方法,其中,所述第一电极(111)包括形成等离子体放电离子源的一对电极构件。高能粒子源,包括:真空室(110),其包括第一电极(111)和第二电极(112),所述第一电极形成等离子体离子源,该等离子体离子源能够产生离子等离子体并提供等离子体离子显影。在朝向所述第二电极的所述腔室中;连接到所述第一电极以向等离子体离子源供电的离子源的触发装置(131);耦合到所述第一和第二电极的高压发生器(132);以及;控制和监视的框(140),以确保响应于所述等离子体离子源的激发而在所述第一和第二电极之间提供高压短脉冲,所述离子源的所述触发装置在所述时间间隔内离子等离子体处于过渡状态,在距所述第二电极一定距离处有空间分布的离子或电子,从而使所述分布的离子或电子向所述第二电极加速并产生高能带电粒子的能量通量,以克服与空间电荷相关的电流极限(传统的真空二极管); 7。 7.根据权利要求6所述的源,其中,由核或电磁反应“束/靶”产生的所述高能粒子出现在所述加速的离子或电子与所述第二电极(112)之间; 8。 7.根据权利要求6所述的源,其中,所述第二电极(112)是半透明的栅格结构,并且所述高能粒子是直接穿过所述第二电极的等离子体离子或电子。 7.根据权利要求6所述的源,其中,所述块(140)所述管理和控制可操作以在相对于所述离子等离子体产生的预定时间延迟之后启动所述高压脉冲。 11.根据权利要求9所述的源,其中,所述时间延迟是至少基于所述电压脉冲的电平,所述电极的几何形状以及它们之间的距离以及所述腔室中的压力来确定的; 11。 11.根据权利要求6-10中任一项所述的源,其中,所述第一电极(111)包括形成等离子体放电离子源的一对电极构件。

著录项

  • 公开/公告号RU2009107215A

    专利类型

  • 公开/公告日2010-09-10

    原文格式PDF

  • 申请/专利权人 САЖ ИННОВАСЬОН ИНК. (MU);

    申请/专利号RU20090107215

  • 发明设计人 ЧОЙ ПИТЕР (FR);

    申请日2007-07-25

  • 分类号H05H3/06;

  • 国家 RU

  • 入库时间 2022-08-21 18:30:01

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