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    • 13. 发明申请
    • METHOD AND APPARATUS FOR CONTROLLING PLASMA UNIFORMITY
    • 用于控制等离子体均匀性的方法和装置
    • US20090197015A1
    • 2009-08-06
    • US12344210
    • 2008-12-24
    • Jozef KudelaGaku FurutaCarl A. SorensenSoo Young ChoiJohn M. White
    • Jozef KudelaGaku FurutaCarl A. SorensenSoo Young ChoiJohn M. White
    • C23C16/513
    • H01J37/32623C23C16/345C23C16/5096H01J37/32082
    • Systems, methods, and apparatus involve a plasma processing chamber for depositing a film on a substrate. The plasma processing chamber includes a lid assembly having a ground plate, a backing plate, and a non-uniformity existing between the ground plate and the backing plate. The non-uniformity may interfere with RF wave uniformity and cause an impedance imbalance between portions of the ground plate and backing plate. The non-uniformity may include a structure or a reduced spacing of non-uniform surfaces. A reduced spacing of non-uniform surfaces may exist where a first distance between the ground plate and the backing plate at a first end is different from a second distance between the ground plate and the backing plate at a second end. The structure may be from 2 cm to 10 cm thick, cover from 20% to 50% of the backing plate, and be located away from a discontinuity existing inside the chamber.
    • 系统,方法和装置包括用于在基板上沉积膜的等离子体处理室。 等离子体处理室包括具有接地板,背板和存在于接地板和背板之间的不均匀性的盖组件。 不均匀性可能会干扰RF波均匀性,并导致接地板和背板的部分之间的阻抗不平衡。 不均匀性可以包括非均匀表面的结构或减小的间隔。 存在不均匀表面的减小的间隔,其中在第一端处的接地板和背板之间的第一距离在第二端处不同于接地板和背板之间的第二距离。 该结构可以是2cm至10cm厚,覆盖背板的20%至50%,并且位于远离存在于腔室内的不连续处。
    • 15. 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。
    • 18. 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。
    • 20. 发明授权
    • Apparatus and methods for a fixed impedance transformation network for use in connection with a plasma chamber
    • 用于与等离子体室结合使用的固定阻抗变换网络的装置和方法
    • US07570130B2
    • 2009-08-04
    • US11179036
    • 2005-07-11
    • Carl A. SorensenJohn M. WhiteSuhail Anwar
    • Carl A. SorensenJohn M. WhiteSuhail Anwar
    • H03H5/00
    • H01J37/32082H01J37/32183
    • In certain embodiments, an apparatus for providing a fixed impedance transformation network for driving a plasma chamber includes a pre-match network adapted to couple between an Active RF match network and a plasma chamber load associated with the plasma chamber. The pre-match network includes (1) a first capacitive element; (2) an inductive element connected in parallel with the first capacitive element to form a parallel circuit that presents a stepped-up impedance to an output of the Active RF match network such that a voltage required to drive the plasma chamber load is reduced; and (3) a second capacitive element coupled to the parallel circuit and adapted to couple to the plasma chamber load. The second capacitive element reduces or cancels at least in part a reactance corresponding to an inductance associated with the plasma chamber load. Numerous other aspects are provided.
    • 在某些实施例中,用于提供用于驱动等离子体室的固定阻抗变换网络的装置包括适于在有源RF匹配网络和与等离子体室相关联的等离子体室负载之间耦合的预匹配网络。 预匹配网络包括(1)第一电容元件; (2)与所述第一电容元件并联连接的电感元件,以形成并联电路,所述并联电路向所述有源RF匹配网络的输出提供升压阻抗,使得驱动所述等离子体室负载所需的电压降低; 和(3)耦合到并联电路并且适于耦合到等离子体室负载的第二电容元件。 第二电容元件至少部分地减小或抵消与等离子体室负载相关联的电感的电抗。 提供了许多其他方面。