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    • 6. 发明授权
    • Cylindrical target with oscillating magnet for magnetron sputtering
    • 圆柱靶用磁控溅射的振荡磁体
    • US07993496B2
    • 2011-08-09
    • US11171054
    • 2005-06-30
    • Klaus HartigSteve E. SmithJohn E. Madocks
    • Klaus HartigSteve E. SmithJohn E. Madocks
    • C23C14/00
    • H01J37/3455H01J37/3405H01J37/3423H01J37/3497
    • In some embodiments, the invention includes a cylindrical cathode target assembly for use in sputtering target material onto a substrate that comprises a generally cylindrical target, means for rotating the target about its axis during a sputtering operation, an elongated magnet carried within the target for generation of a plasma-containing magnetic field exterior to but adjacent the target, a framework for supporting the magnet against rotation within the target, and a power train for causing the magnet to oscillate within and axially of the target in a substantially asynchronous manner to promote generally uniform target utilization along its length, as well as its method of use. In some embodiments, the magnet is oscillated in response to rotation of the target.
    • 在一些实施例中,本发明包括用于将目标材料溅射到基板上的圆柱形阴极靶组件,该基板包括大致圆柱形的靶,用于在溅射操作期间使靶围绕其轴旋转的装置,用于产生的靶内的细长磁体 位于目标外部但邻近目标的等离子体磁场,用于支撑磁体以防止目标内的旋转的框架和用于使磁体以基本上异步的方式在目标内部和轴向振荡的传动系,以促进一般 沿其长度的均匀目标利用率及其使用方法。 在一些实施例中,磁体响应于目标的旋转而振荡。
    • 8. 发明授权
    • Dual plasma beam sources and method
    • 双等离子体束源和方法
    • US07411352B2
    • 2008-08-12
    • US11379349
    • 2006-04-19
    • John E. Madocks
    • John E. Madocks
    • H01J7/24
    • H05H1/46C23C14/32C23C16/513H01J37/3266
    • A pair of plasma beam sources are connected across an AC power supply to alternatively produce an ion beam for depositing material on a substrate transported past the ion beams. Each plasma beam source includes a discharge cavity having a first width and a nozzle extending outwardly therefrom to emit the ion beam. The aperture or outlet of the nozzle has a second width, which second width is less than the first width. An ionizable gas is introduced to the discharge cavity. At least one electrode connected to the AC power supply, alternatively serving as an anode or a cathode, is capable of supporting at least one magnetron discharge region within the discharge cavity when serving as a cathode electrode. A plurality of magnets generally facing one another, are disposed adjacent each discharge cavity to create a magnetic field null region within the discharge cavity.
    • 一对等离子体束源连接在交流电源上,以交替地产生用于在经过离子束传送的衬底上沉积材料的离子束。 每个等离子体束源包括具有第一宽度的排出腔和从其向外延伸以喷射离子束的喷嘴。 喷嘴的孔或出口具有第二宽度,该第二宽度小于第一宽度。 将可电离气体引入到排出腔。 连接到AC电源的替代地用作阳极或阴极的至少一个电极能够在用作阴极时支持放电腔内的至少一个磁控管放电区域。 大体上彼此面对的多个磁体邻近每个排出腔设置,以在排出腔内形成磁场零区域。
    • 9. 发明授权
    • Beam plasma source
    • 光束等离子体源
    • US07327089B2
    • 2008-02-05
    • US10528386
    • 2003-09-19
    • John E. Madocks
    • John E. Madocks
    • H01J7/24
    • H05H1/46H01J27/146H01J37/32009H01J37/32357H01J37/3266H01J2237/0815H05H1/48
    • A plasma source which includes a discharge cavity having a first width, where that discharge cavity includes a top portion, a wall portion, and a nozzle disposed on the top portion and extending outwardly therefrom, where the nozzle is formed to include an aperture extending through the top portion and into the discharge cavity, wherein the aperture has a second width, where the second width is less than the first width. The plasma source further includes a power supply, a conduit disposed in the discharge cavity for introducing an ionizable gas therein, and at least one cathode electrode connected to the power supply, where that cathode electrode is capable of supporting at least one magnetron discharge region within the discharge cavity. The plasma source further includes a plurality of magnets disposed adjacent the wall portion, where that plurality of magnets create a null magnetic field point within the discharge cavity.
    • 一种等离子体源,其包括具有第一宽度的排出腔,其中所述排出腔包括顶部,壁部分和设置在顶部上并从其向外延伸的喷嘴,其中所述喷嘴形成为包括延伸穿过的孔 顶部并进入排出腔,其中孔具有第二宽度,其中第二宽度小于第一宽度。 等离子体源还包括电源,设置在放电腔中的用于在其中引入可电离气体的导管和连接到电源的至少一个阴极,其中阴极能够支撑至少一个磁控管放电区域 放电腔。 等离子体源还包括邻近壁部设置的多个磁体,其中多个磁体在放电腔内形成零磁场点。