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    • 5. 发明申请
    • MAGNETRON PLASMA APPARATUS
    • MAGNETRON等离子体设备
    • US20170047204A1
    • 2017-02-16
    • US15335584
    • 2016-10-27
    • BB PLASMA DESIGN AB
    • Ladislav BARDOSHana BARANKOVA
    • H01J37/34C23C14/34C23C14/35H01J37/32
    • H01J37/3405C23C14/3407C23C14/35C23C14/352H01J37/32596H01J37/3402H01J37/342H01J37/3423H01J37/3438H01J37/345
    • A magnetron plasma apparatus boosted by hollow cathode plasma includes at least one electrically connected pair of a first hollow cathode plate and a second hollow cathode plate placed opposite to each other at a separation distance of at least 0.1 mm and having an opening following an outer edge of a sputter erosion zone on a magnetron target so that a magnetron magnetic field forms a perpendicular magnetic component inside a hollow cathode slit between plates and, wherein the plates and are connected to a first electric power generator together with the magnetron target to generate a magnetically enhanced hollow cathode plasma in at least one of a first working gas distributed in the hollow cathode slit and a second working gas admitted outside the slit in contact with a magnetron plasma generated in at least one of the first working gas and the second working gas.
    • 由空心阴极等离子体增强的磁控管等离子体装置包括至少一个电连接的一对第一中空阴极板和第二中空阴极板,该第一空心阴极板和第二中空阴极板以至少0.1mm的间隔距离彼此相对放置, 在磁控管靶上形成溅射侵蚀区,使得磁控管磁场在板之间的中空阴极狭缝内形成垂直的磁性部件,并且其中板与磁控管靶一起连接到第一发电机,以产生磁性 分散在中空阴极狭缝中的第一工作气体中的至少一个中的增强的空心阴极等离子体以及与在第一工作气体和第二工作气体中的至少一个中产生的磁控管等离子体接触的狭缝外部的第二工作气体。
    • 8. 发明授权
    • Scalable and uniformity controllable diffusion plasma source
    • 可扩展和均匀可控扩散等离子体源
    • US09431218B2
    • 2016-08-30
    • US14209695
    • 2014-03-13
    • Tokyo Electron Limited
    • Jianping ZhaoLee ChenRadha SundararajanMerritt Funk
    • H05B39/00H01J37/32
    • H01J37/32357H01J37/32422H01J37/32596
    • A method of treating a substrate with plasma is described. In particular, the method includes disposing a substrate in a plasma processing system, disposing a hollow cathode plasma source including at least one hollow cathode within the plasma processing system, and disposing a grid between the cathode outlet of the plurality of hollow cathodes and the substrate. The method further includes electrically coupling the grid to electrical ground, coupling a voltage to the at least one hollow cathode relative to electrical ground, and generating plasma in hollow cathode by ion-induced secondary electron emission of energetic electrons that move along a first trajectory, and diffusing lower energy electrons along a second trajectory across a first region of the interior space between the cathode outlet and the grid, through the grid, and into a second region of the interior space in fluid contact with the substrate.
    • 描述了用等离子体处理衬底的方法。 特别地,该方法包括在等离子体处理系统中设置衬底,在等离子体处理系统内设置包括至少一个中空阴极的中空阴极等离子体源,并且在多个中空阴极的阴极出口和衬底之间设置栅极 。 该方法还包括将电网电耦合到电接地,将电压相对于电接地耦合​​到至少一个空心阴极,以及通过离子诱导的沿着第一轨迹移动的能量电子的二次电子发射在空心阴极中产生等离子体, 并且沿着第二轨迹穿过阴极出口和格栅之间的内部空间的第一区域,穿过网格,并且进一步流体地与衬底接触的内部空间的第二区域中扩散较低能量的电子。
    • 9. 发明申请
    • METHOD AND APPARATUS FOR PLASMA IGNITION IN HIGH VACUUM CHAMBERS
    • 高真空气体中等离子体点火的方法与装置
    • US20160163519A1
    • 2016-06-09
    • US14982260
    • 2015-12-29
    • XEI Scientic, Inc.
    • Ronald A. VaneMichael Cable
    • H01J37/32
    • H01J37/32862H01J37/32082H01J37/32357H01J37/32449H01J37/32596H01J2237/335
    • A new method and apparatus is described for igniting a plasma from high vacuum. The ignition method uses a small, short term and quick rise in gas flow into plasma chamber while being excited by RF power to ignite the plasma and then drops the gas flow to fixed input flow rate to maintain the plasma. This plasma starting technique does not use electronic means for ignition. The associated apparatus has a gas buffer chamber in fluid communication with the gas source and the plasma chamber, the gas buffer chamber having a small volume gas that is refilled when the device is off. A flow restriction between the gas source and the gas buffer chamber has a maximum flow rate therethrough of 30 sccm (standard cubic centimeters per minute) or less. A valve between the plasma chamber and the gas buffer chamber permits flow between the gas chamber and the plasma chamber, wherein, upon opening the valve, gas is admitted into the plasma chamber and pressure in the plasma chamber rises temporarily causing plasma ignition if the plasma excitation device is energized. The flow restriction maintains the gas flow during plasma operation to maintain a pressure between approximately 0.5 Pa and approximately 6-7 Pa.
    • 描述了一种用于从高真空点燃等离子体的新方法和装置。 点火方法在通过RF功率激发以点燃等离子体然后将气体流量降至固定输入流量以维持等离子体时,使用气体流入等离子体室的小的,短期的和快速的上升。 该等离子体启动技术不使用电子点火装置。 相关联的装置具有与气体源和等离子体室流体连通的气体缓冲室,气体缓冲室具有小的体积气体,当装置关闭时,其被重新填充。 气体源和气体缓冲室之间的流量限制具有30sccm(标准立方厘米每分钟)或更小的最大流速。 等离子体室和气体缓冲室之间的阀允许在气体室和等离子体室之间流动,其中,在打开阀时,气体被允许进入等离子体室,等离子体室中的压力暂时升高,如果等离子体 励磁装置通电。 流量限制保持等离子体操作期间的气体流动,以将压力保持在约0.5Pa和约6-7Pa之间。
    • 10. 发明申请
    • Method and Device for Generating an Electrical Discharge
    • 用于产生放电的方法和装置
    • US20160118231A1
    • 2016-04-28
    • US14923303
    • 2015-10-26
    • CemeCon AG
    • Walter May
    • H01J37/34C23F4/04C23C14/35
    • H01J37/3411C23C14/35C23F4/04H01J37/3244H01J37/32596H01J37/3405H05H1/48
    • A device and method for generating an electrical discharge are described. A first electrode (30) is operated to be a cathode relative to a second electrode (16). A gas is introduced into the chamber (14) by the first electrode (30). The first electrode (30) has a closed antechamber (32) with a metal wall (34). A tube (36) consisting of a different material than the wall (34) is provided through which the gas from the antechamber (32) is conducted into the chamber (14). A front portion of the tube (36) is embedded in the wall (34) of the antechamber (32). In its rear portion, the tube (36) has a free end projecting into the antechamber (32). A stable electrical discharge can be generated thereby in a particularly easy manner.
    • 描述了一种用于产生放电的装置和方法。 第一电极(30)相对于第二电极(16)操作为阴极。 通过第一电极(30)将气体引入室(14)。 第一电极(30)具有带有金属壁(34)的封闭的前室(32)。 提供由不同于壁(34)的材料构成的管(36),来自前厅(32)的气体通过该导管进入腔室(14)。 管(36)的前部嵌入前厅(32)的壁(34)中。 在其后部,管(36)具有伸入前厅(32)的自由端。 由此可以特别容易地产生稳定的放电。