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    • 31. 发明申请
    • Asymmetrical RF Drive for Electrode of Plasma Chamber
    • 等离子室电极的非对称RF驱动
    • US20090159423A1
    • 2009-06-25
    • US12343519
    • 2008-12-24
    • Jozef KudelaCarl A. SorensenSoo Young ChoiJohn M. White
    • Jozef KudelaCarl A. SorensenSoo Young ChoiJohn M. White
    • H05H1/00H01L21/3065B23H7/14
    • H01L21/02B44C1/227C23C16/513H01J37/32091H01J37/32577H01L21/02104
    • RF power is coupled to one or more RF drive points (50-56) on an electrode (20-28) of a plasma chamber such that the level of RF power coupled to the RF drive points (51-52, 55-56) on the half (61) of the electrode that is closer to the workpiece passageway (12) exceeds the level of RF power coupled to the RF drive points (53-54), if any, on the other half (62) of the electrode. Alternatively, RF power is coupled to one or more RF drive points on an electrode of a plasma chamber such that the weighted mean of the drive point positions is between the center (60) of the electrode and the workpiece passageway. The weighted mean is based on weighting each drive point position by the time-averaged level of RF power coupled to that drive point position. The invention offsets an increase in plasma density that otherwise would exist adjacent the end of the electrode closest to the passageway.
    • RF功率耦合到等离子体室的电极(20-28)上的一个或多个RF驱动点(50-56),使得耦合到RF驱动点(51-52,55-56)的RF功率的电平 更靠近工件通道(12)的电极的一半(61)超过了电极的另一半(62)上耦合到RF驱动点(53-54)的RF功率的水平(如果有的话) 。 或者,RF功率耦合到等离子体室的电极上的一个或多个RF驱动点,使得驱动点位置的加权平均值在电极的中心(60)和工件通道之间。 加权平均值基于通过耦合到该驱动点位置的RF功率的时间平均水平来加权每个驱动点位置。 本发明抵消等离子体密度的增加,否则其将邻近电极最靠近通道的端部存在。
    • 37. 发明授权
    • Plasma uniformity control by gas diffuser hole design
    • 通过气体扩散器孔设计的等离子体均匀性控制
    • US08083853B2
    • 2011-12-27
    • US10889683
    • 2004-07-12
    • Soo Young ChoiJohn M. WhiteQunhua WangLi HouKi Woon KimShinichi KuritaTae Kyung WonSuhail AnwarBeom Soo ParkRobin L. Tiner
    • Soo Young ChoiJohn M. WhiteQunhua WangLi HouKi Woon KimShinichi KuritaTae Kyung WonSuhail AnwarBeom Soo ParkRobin L. Tiner
    • C23C16/00C23C16/455H01L21/3065
    • H01J37/3244C23C16/345C23C16/455C23C16/45565C23C16/5096H01J37/32082H01J37/32091H01J37/32541H01J37/32596H01J2237/327H01J2237/3321H01J2237/3323H01J2237/3325Y10T29/49885Y10T29/49996
    • Embodiments of a gas diffuser plate for distributing gas in a processing chamber are provided. The gas distribution plate includes a diffuser plate having an upstream side and a downstream side, and a plurality of gas passages passing between the upstream and downstream sides of the diffuser plate. The gas passages include hollow cathode cavities at the downstream side to enhance plasma ionization. The depths, the diameters, the surface area and density of hollow cathode cavities of the gas passages that extend to the downstream end can be gradually increased from the center to the edge of the diffuser plate to improve the film thickness and property uniformity across the substrate. The increasing diameters, depths and surface areas from the center to the edge of the diffuser plate can be created by bending the diffuser plate toward downstream side, followed by machining out the convex downstream side. Bending the diffuser plate can be accomplished by a thermal process or a vacuum process. The increasing diameters, depths and surface areas from the center to the edge of the diffuser plate can also be created computer numerically controlled machining. Diffuser plates with gradually increasing diameters, depths and surface areas of the hollow cathode cavities from the center to the edge of the diffuser plate have been shown to produce improved uniformities of film thickness and film properties.
    • 提供了用于在处理室中分配气体的气体扩散板的实施例。 气体分配板包括具有上游侧和下游侧的扩散板,以及在扩散板的上游侧和下游侧之间通过的多个气体通路。 气体通道包括在下游侧的中空阴极腔,以增强等离子体电离。 延伸到下游端的气体通道的空心阴极腔的深度,直径,表面积和密度可以从扩散板的中心到边缘逐渐增加,以改善衬底上的膜厚度和性能均匀性 。 从扩散板的中心到边缘的直径,深度和表面积的增加可以通过向下游侧弯曲扩散板,然后在凸出的下游侧加工出来。 扩散板的弯曲可以通过热处理或真空工艺来实现。 从扩散板的中心到边缘的直径,深度和表面积的增加也可以用计算机数字控制加工。 具有从扩散板的中心到边缘的中空阴极腔的直径逐渐增加,深度和表面积逐渐增大的扩散板已被证明可以产生改善的膜厚度和膜性质的均匀性。
    • 39. 发明授权
    • Asymmetrical RF drive for electrode of plasma chamber
    • 等离子体室用电极的非对称RF驱动
    • US08343592B2
    • 2013-01-01
    • US12343519
    • 2008-12-24
    • Jozef KudelaCarl A. SorensenSoo Young ChoiJohn M. White
    • Jozef KudelaCarl A. SorensenSoo Young ChoiJohn M. White
    • H05H1/24H01L21/306C23C16/00
    • H01L21/02B44C1/227C23C16/513H01J37/32091H01J37/32577H01L21/02104
    • RF power is coupled to one or more RF drive points (50-56) on an electrode (20-28) of a plasma chamber such that the level of RF power coupled to the RF drive points (51-52, 55-56) on the half (61) of the electrode that is closer to the workpiece passageway (12) exceeds the level of RF power coupled to the RF drive points (53-54), if any, on the other half (62) of the electrode. Alternatively, RF power is coupled to one or more RF drive points on an electrode of a plasma chamber such that the weighted mean of the drive point positions is between the center (60) of the electrode and the workpiece passageway. The weighted mean is based on weighting each drive point position by the time-averaged level of RF power coupled to that drive point position. The invention offsets an increase in plasma density that otherwise would exist adjacent the end of the electrode closest to the passageway.
    • RF功率耦合到等离子体室的电极(20-28)上的一个或多个RF驱动点(50-56),使得耦合到RF驱动点(51-52,55-56)的RF功率的电平 更靠近工件通道(12)的电极的一半(61)超过了电极的另一半(62)上耦合到RF驱动点(53-54)的RF功率的水平(如果有的话) 。 或者,RF功率耦合到等离子体室的电极上的一个或多个RF驱动点,使得驱动点位置的加权平均值在电极的中心(60)和工件通道之间。 加权平均值基于通过耦合到该驱动点位置的RF功率的时间平均水平来加权每个驱动点位置。 本发明抵消等离子体密度的增加,否则其将邻近电极最靠近通道的端部存在。
    • 40. 发明申请
    • RPSC AND RF FEEDTHROUGH
    • RPSC和RF FEEDTHROUGH
    • US20090151636A1
    • 2009-06-18
    • US12271613
    • 2008-11-14
    • John M. WhiteBradley O. StimsonJozef Kudela
    • John M. WhiteBradley O. StimsonJozef Kudela
    • C23C16/513C23C16/511
    • H01J37/32697H01J37/32091H01J37/32192H01J37/32357H01J37/32862
    • The present invention generally comprises an apparatus having an RF choke and a remote plasma source combined into a single unit. Process gases may be introduced to the chamber via the showerhead assembly which may be driven as an RF electrode. The gas feed tube may provide process gases and the cleaning gases to the process chamber. The inside of the gas feed tube may remain at a zero RF field to avoid premature gas breakdown within the gas feed tube that may lead to parasitic plasma formation between the gas source and the showerhead during processing. Igniting the cleaning gas plasma within the gas feed tube permits the plasma to be ignited closer to the processing chamber. Thus, RF current travels along the outside of the apparatus during deposition and microwave current ignites a plasma within the apparatus before feeding the plasma to the processing chamber.
    • 本发明通常包括具有组合成单个单元的RF扼流圈和远程等离子体源的装置。 工艺气体可以经由可被作为RF电极驱动的喷头组件引入室。 气体供给管可以将处理气体和清洁气体提供给处理室。 气体供给管的内部可以保持在零RF场,以避免气体进料管内的过早气体击穿,这可能在处理期间导致气体源和喷头之间的寄生等离子体形成。 点燃气体供给管内的清洁气体等离子体允许等离子体更靠近处理室被点燃。 因此,RF电流在沉积期间沿着设备的外部行进,并且在将等离子体馈送到处理室之前,微波电流点燃设备内的等离子体。