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    • 5. 发明授权
    • Metal ion plasma generator having magnetic field forming device located
such that a triggering is between the magnetic field forming device and
an anode
    • 具有磁场形成装置的金属离子等离子体发生器,其定位成使得在磁场形成装置和阳极之间触发
    • US5896012A
    • 1999-04-20
    • US908985
    • 1997-08-08
    • Jun MunemasaAlexander ElkindJames R Treglio
    • Jun MunemasaAlexander ElkindJames R Treglio
    • C23C14/24C23C14/32H01J27/04H01J37/32H05B31/026H01J7/24
    • H01J37/32055C23C14/325H01J27/04H01J37/3266
    • When a trigger discharge between a metal cathode and a trigger ring induces a vacuum-arc discharge between the cathode an anode, which vaporizes the substances of the cathode surface to produce a metal ion plasma, setting the pulse length of the arc pulse applied between the cathode and the anode to 1 msec or longer will soon short-circuit between the cathode and the trigger ring due to the vaporized substances deposited on the surface of the insulating ring. In order to solve this problem, a permanent magnet 36 for forming a magnetic field across a space between the anode 26 and the cathode 34 is provided close to the rear side of the trigger ring 35 so as to guide the substances vaporized from the cathode 34 toward the anode 26. Thereby, a longer continuous operation can be done with setting the arc pulse longer. moreover, since the permanent magnet 36 is provided at the foregoing position, the magnet does not receive a thermal load by the vacuum-arc discharge, which maintains a stable operation and makes the total construction compact.
    • 当金属阴极和触发环之间的触发放电在阴极和阴极表面的物质蒸发以产生金属离子等离子体的阴极之间引起真空电弧放电时,设置施加在金属阴极和触发环之间的电弧脉冲的脉冲长度 阴极和阳极至1毫秒或更长时间将由于沉积在绝缘环表面上的汽化物质而在阴极和触发环之间短路。 为了解决这个问题,在触发环35的后侧附近设置用于在阳极26和阴极34之间的空间形成磁场的永磁体36,以引导从阴极34蒸发的物质 从而可以通过更长时间地设置电弧脉冲来进行更长的连续操作。 此外,由于永久磁铁36设置在上述位置,所以磁体不会受到真空电弧放电的热负荷的影响,从而保持了稳定的动作,使总体结构紧凑。
    • 8. 发明授权
    • Penning discharge ion source with self-cleaning aperture
    • Penning放电离子源具有自清洁孔径
    • US4344019A
    • 1982-08-10
    • US205398
    • 1980-11-10
    • Basil F. GavinRobert A. MacGillRaymond K. Thatcher
    • Basil F. GavinRobert A. MacGillRaymond K. Thatcher
    • H01J27/04
    • H01J27/04
    • An ion source of the Penning discharge type having a self-cleaning aperture is provided by a second dynode (24) with an exit aperture (12) in a position opposite a first dynode 10a, from which the ions are sputtered, two opposing cathodes (14, 16), each with an anode (18, 20) for accelerating electrons emitted from the cathodes into a cylindrical space defined by the first and second dynode. A support gas maintained in this space is ionized by the electrons. While the cathodes are supplied with a negative pulse to emit electrons, the first dynode is supplied with a negative pulse (e.g., -300 V) to attract atoms of the ionized gas (plasma). At the same time, the second dynode may also be supplied with a small voltage that is negative with respect to the plasma (e.g., -5 V) for tuning the position of the plasma miniscus for optimum extraction geometry. When the negative pulse to the first dynode is terminated, the second dynode is driven strongly negative (e.g., -600 V) thereby allowing heavy sputtering to take place for a short period to remove virtually all of the atoms deposited on the second dynode from material sputtered off the first dynode. An extractor (22) immediately outside the exit aperture of the second dynode is maintained at ground potential during this entire period of sputtering while the anode, dynode and cathode reference voltage is driven strongly positive (about +20 kV to +30 kV) so that ions accelerated through the aperture will be at ground potential. In that manner, material from the first dynode deposited on the second dynode will be sputtered, in time, to add to the ion beam. Atoms sputtered from the second dynode which do not become ionized and exit through the slit will be redeposited on the first dynode, and hence recycled for further ion beam generation during subsequent operating cycles.
    • 具有自清洁孔径的Penning放电型离子源由具有出口孔(12)的第二倍增电极(24)提供在与第一倍增电极10a相对的位置,离子被溅射出来,两个相对的阴极 每个具有用于将从阴极发射的电子加速到由第一和第二倍增电极限定的圆柱形空间中的阳极(18,20)。 保持在该空间中的支撑气体被电子电离。 当阴极被提供有负脉冲以发射电子时,第一倍增电极被提供有负脉冲(例如,-300V)以吸引电离气体(等离子体)的原子。 同时,也可以向第二倍增电极提供相对于等离子体为负的小电压(例如,-5V),用于调整等离子体液面的位置以获得最佳的提取几何形状。 当第一倍增极的负脉冲终止时,第二倍增电极被强烈地负(例如,-600V),从而允许在很短的时间内发生重的溅射,从而从材料中去除几乎所有沉积在第二倍增极上的原子 溅出第一个dynode。 在整个溅射期间,紧邻第二倍增电极的出口孔外面的提取器(22)保持接地电位,而阳极,倍增极和阴极参考电压被强烈地驱动(约+ 20kV至+ 30kV),使得 通过孔径加速的离子将处于地电位。 以这种方式,沉积在第二倍增电极上的第一倍增电极的材料将被及时地溅射以添加到离子束。 从第二倍增极溅射的不会离子化并通过狭缝出射的原子将重新沉积在第一倍增极上,因此在随后的操作循环期间再循环用于进一步的离子束产生。