子分类：
| 序号 | 专利名 | 申请号 | 申请日 | 公开（公告）号 | 公开（公告）日 | 发明人 |
|---|---|---|---|---|---|---|
| 1 | 控制流体流量用静电流体加速器以及控制流体流量的方法 | CN200580024277.7 | 2005-05-18 | CN1993796A | 2007-07-04 | 伊格尔·A·克里希塔福维奇; 弗拉基米尔·L·戈罗别茨 |
| 本发明涉及一种静电流体加速器及其操作方法，包括至少两个同步供电的级，其中一级的最后或最末电极的瞬时电压保持为和沿空气流方向下一级的紧邻初始或最前端电极的瞬时电压基本上相同。单个电源或同步且相位受控的电源提供高压电力到每个级，以使得提供到对应电极的电源的相位和振幅在时间上对准。频率和相位控制使得相邻级紧密靠近的距离是级内的电极间距离的1至2倍，以及，无论如何，最小化或避免从一个级的电晕放电电极至相邻级的电极之间产生负效电晕电流。相邻级的电晕放电电极可以水平对齐，所有级的补充集电电极都在其中类似地水平对齐以及水平偏离于电晕放电电极。 | ||||||
| 2 | 高压加速器的高压舱结构 | CN201310685439.8 | 2013-12-16 | CN103928281B | 2017-08-25 | 黄永章 |
| 本发明涉及高压领域，其公开了一种高压加速器的高压舱结构,包括一个高电压舱，带电粒子发生器，加速管，束流输运线和目标靶;所述高电压舱的内部为空心腔体，所述带电粒子发生器设置在所述空心腔体内；所述高电压舱设置在高的电位以协助加速从带电粒子发生器出来的电子；高电压舱被包围在一个接地的外壳内；所述高电压舱的边缘的外部附近设置有绝缘导体。本发明的有益效果是：根据高电压舱结构与周围的接地外壳的空气间隔的不同来设置绝缘导体的位置，从而进一步提高高电压舱的最高承受电压。 | ||||||
| 3 | 电子束装置 | CN93103626.7 | 1993-03-27 | CN1079335A | 1993-12-08 | H·-G·马修斯; W·施明克 |
| 一种电子束装置，包括阴极(1)、阳极(3)和集电极(4)。阴极产生沿电子束轴线(5)传播的高功率电子束；阳极沿所述轴线设在阴极后面；集电极沿所述轴线设在阳极后面，并由在所述轴线上相继排列的处于较低电位级的若干集电极级(6)构成，用以降低电子束中电子的速度。电位供应电路采用高压直流电源(13)，该电源由多个开关级(S1、……、S6)组成，以构成可切换的中压源，其输出端串联连接。集电极级的分级电位由开关级间的相应抽头提供。 | ||||||
| 4 | 高压加速器的高压舱结构 | CN201310685439.8 | 2013-12-16 | CN103928281A | 2014-07-16 | 黄永章 |
| 本发明涉及高压领域，其公开了一种高压加速器的高压舱结构，包括一个高电压舱，带电粒子发生器，加速管，束流输运线和目标靶；所述高电压舱的内部为空心腔体，所述带电粒子发生器设置在所述空心腔体内；所述高电压舱设置在高的电位以协助加速从带电粒子发生器出来的电子；高电压舱被包围在一个接地的外壳内；所述高电压舱的边缘的外部附近设置有绝缘导体。本发明的有益效果是：根据高电压舱结构与周围的接地外壳的空气间隔的不同来设置绝缘导体的位置，从而进一步提高高电压舱的最高承受电压。 | ||||||
| 5 | 强流直流质子加速器 | CN200980131131.0 | 2009-08-11 | CN102119584B | 2014-02-12 | 马歇尔·R·克莱兰德; 理查德·A·加洛韦; 伦纳德·德桑图; 伊维斯·钟恩 |
| 提供了一种能够在高能下使强流质子束加速的直流加速器系统。加速器系统包括直流高压、大电流电源，抽空的离子加速管，质子离子源，偶极分析磁铁以及位于高压终端的真空泵。可基于多种应用，例如硼中子俘获疗法(BNCT)应用、NRA应用、以及硅石分裂，将强流、高能直流质子束引向多个靶。 | ||||||
| 6 | 强流直流质子加速器 | CN200980131131.0 | 2009-08-11 | CN102119584A | 2011-07-06 | 马歇尔·R·克莱兰德; 理查德·A·加洛韦; 伦纳德·德桑图; 伊维斯·钟恩 |
| 提供了一种能够在高能下使强流质子束加速的直流加速器系统。加速器系统包括直流高压、大电流电源，抽空的离子加速管，质子离子源，偶极分析磁铁以及位于高压终端的真空泵。可基于多种应用，例如硼中子俘获疗法(BNCT)应用、NRA应用、以及硅石分裂，将强流、高能直流质子束引向多个靶。 | ||||||
| 7 | HIGH-CURRENT DC PROTON ACCELERATOR | EP09791382.6 | 2009-08-11 | EP2329692A1 | 2011-06-08 | CLELAND, Marshall, R.; GALLOWAY, Richard, A.; DESANTO, Leonard; JONGEN, Yves |
| A dc accelerator system able to accelerate high currents of proton beams at high energies is provided. The accelerator system includes a dc high-voltage, high-current power supply, an evacuated ion accelerating tube, a proton ion source, a dipole analyzing magnet and a vacuum pump located in the high-voltage terminal. The high-current, high-energy dc proton beam can be directed to a number of targets depending on the applications such as boron neutron capture therapy BNCT applications, NRA applications, and silicon cleaving. | ||||||
| 8 | Elektronenstrahl-Vorrichtung | EP93101880.8 | 1993-02-06 | EP0563543B1 | 1996-08-28 | Mathews, Hans-Günter,Dr.; Schminke, Wolfram, Dr. |
| 9 | VERFAHREN ZUM BESCHLEUNIGEN ELEKTRISCH GELADENER TEILCHEN | EP93906431.0 | 1993-03-18 | EP0631712A1 | 1995-01-04 | SCHULTHEISS, Christoph; KONIJNENBERG, Martin; SCHWALL, Markus |
| A process for accelerating electrically charged particles and a particle accelerator for applying the process are diclosed. The beam thus generated has a high degree of intensity and convergence and is suitable for uniformly depositing a material on a substrate. Similarly, it is useful for generating light of different spectral regions. | ||||||
| 10 | AN ELECTROSTATIC FLUID ACCELERATOR FOR AND A METHOD OF CONTROLLING FLUID FLOW | EP05750980 | 2005-05-18 | EP1759401A4 | 2012-02-01 | KRICHTAFOVITCH IGOR A; GOROBETS VLADIMIR L |
| 11 | Accélérateur électrostatique d'électrons | EP90402251.4 | 1990-08-06 | EP0412896A1 | 1991-02-13 | Roche, Michel |
Accélérateur électrostatique possédant un tube accélérateur d'électrons (44) dont la tension d'accélération est répartie sur sa longueur par un multiplicateur de tension de type Greinacher alimenté par un signal électrique dont la fréquence est contenue dans une gamme allant de 0,5 à 1 MHz. Une enceinte pressurisée (20) contient les éléments principaux du dispositif. Application à la stérilisation, à la désinfection, à la débactérisation et à tout autre utilisation de rayonnements ionisants. |
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| 12 | Electrostatic ion accelerator | EP87307575.8 | 1987-08-27 | EP0300105A2 | 1989-01-25 | Shefer, Ruth; Klinkowstein,Robert Edward |
A high current (0.2 to at least 2 milliamperes), low-energy (2.2 to 4 MV) ion beam is generated and is utilized to produce clinically significant quantities of medical isotopes useful in applications such as positron emission tomography. For a preferred embodiment, a tandem accelerator is utilized. Negative ions (202) generated by a high current negative-ion source (200) are accelerated by an electrostatic accelerator in which the necessary high voltage is produced by a solid state power supply. The accelerated ions then enter a stripping cell (212) which removes electrons from the ions, converting them into positive ions. The positive ions (218) are then accelerated to a target which is preferably at ground potential. For a preferred embodiment, the solid state power supply utilized to develop the required voltages is a cascade rectifier power supply (206) which is coaxial with the accelerator between the ion source (200) and the stripper (212), and is designed to have a voltage gradient which substantially matches the maximum voltage gradient of the accelerator. |
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| 13 | High-current DC proton accelerator | JP2011523098 | 2009-08-11 | JP2012500454A | 2012-01-05 | ギャロウェー，リチャード，エー．; クレランド，マーシャル，アール．; デサント，レオナルド; ヨンゲン，イヴ |
| A dc accelerator system able to accelerate high currents of proton beams at high energies is provided. The accelerator system includes a dc high-voltage, high-current power supply, an evacuated ion accelerating tube, a proton ion source, a dipole analyzing magnet and a vacuum pump located in the high-voltage terminal. The high-current, high-energy dc proton beam can be directed to a number of targets depending on the applications such as boron neutron capture therapy BNCT applications, NRA applications, and silicon cleaving. | ||||||
| 14 | Acceleration methods and particle decelerator of charged particles | JP51616993 | 1993-03-18 | JP2831468B2 | 1998-12-02 | SHURUTAISU KURISUTOFU; KONIINENBERUKU MARUTEIN; SHUARU MARUKUSU |
| 15 | Electron beam device | JP6953093 | 1993-03-29 | JPH0684474A | 1994-03-25 | HANSUUGIYUNTAA MATEUSU; BUORUFURAMU SHIYUMINKE |
| PURPOSE: To provide an electron beam device to improve function efficiency at a technically marginal cost and to enhance reliability and safety. CONSTITUTION: A collector 4 includes several collector stages 6 arranged back and forth in a beam axis direction. The collector stages 6 have potential to be reduced by every stage. A feeding part having a high voltage direct current feeding part 13 comprises several switch stages S1,..., S6 of the same type, and these switch stages S1,..., S6 are constituted as switchable intermediate voltage sources whose output sides are connected in series. The multistage potential of the collector stages 6 is generated by a corresponding tap between the switch stages Si and Si+1 (i=1,..., 5) of the high voltage direct current feeding part 13. | ||||||
| 16 | JPH04504483A - | JP50218090 | 1990-02-01 | JPH04504483A | 1992-08-06 | |
| 17 | JPS57500532A - | JP50114280 | 1980-05-05 | JPS57500532A | 1982-03-25 | |
| 18 | HIGH-CURRENT DC PROTON ACCELERATOR | EP09791382.6 | 2009-08-11 | EP2329692B1 | 2018-03-21 | CLELAND, Marshall, R.; GALLOWAY, Richard, A.; DESANTO, Leonard; JONGEN, Yves |
| A dc accelerator system able to accelerate high currents of proton beams at high energies is provided. The accelerator system includes a dc high-voltage, high-current power supply, an evacuated ion accelerating tube, a proton ion source, a dipole analyzing magnet and a vacuum pump located in the high-voltage terminal. The high-current, high-energy dc proton beam can be directed to a number of targets depending on the applications such as boron neutron capture therapy BNCT applications, NRA applications, and silicon cleaving. | ||||||
| 19 | AN ELECTROSTATIC FLUID ACCELERATOR FOR AND A METHOD OF CONTROLLING FLUID FLOW | EP05750980.4 | 2005-05-18 | EP1759401A2 | 2007-03-07 | KRICHTAFOVITCH, Igor, A.; GOROBETS, Vladimir, L. |
| An electrostatic fluid acceleration and method of operation thereof includes at least two synchronously powered stages with final or rear-most electrodes of one stage maintained at substantially the same instantaneous voltage as the immediately adjacent initial or forward-most electrodes of a next stage in an airflow direction. A single power supply or synchronized and phase controlled power supplies provide high voltage power to each of the stages such that both the phase and amplitude of the electric power applied to the corresponding electrodes are aligned in time. The frequency and phase control allows neighboring stages to be closely spaced at a distance of from 1 to 2 times an inter-electrode distance within a stage, and, in any case, minimizing or avoiding production of a back corona current from a corona discharge electrode of one stage to an electrode of a neighboring stage. Corona discharge electrodes of neighboring stages may be horizontally aligned, complementary collector electrodes of all stages being similarly horizontally aligned between and horizontally offset from the corona discharge electrodes. | ||||||
| 20 | VERFAHREN ZUM BESCHLEUNIGEN ELEKTRISCH GELADENER TEILCHEN | EP93906431.7 | 1993-03-18 | EP0631712B1 | 1998-05-20 | SCHULTHEISS, Christoph; KONIJNENBERG, Martin; SCHWALL, Markus |
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