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    • 31. 发明授权
    • Two dimensional stationary beam profile and angular mapping
    • 二维静止波束剖面和角度映射
    • US06872953B1
    • 2005-03-29
    • US10850298
    • 2004-05-20
    • Victor M. Benveniste
    • Victor M. Benveniste
    • H01J37/317
    • H01J37/3171H01J2237/244H01J2237/24507H01J2237/24528H01J2237/304H01J2237/31703
    • An ion beam uniformity detector of the present invention includes a number of horizontal rods and a number of vertical rods placed on parallel planes and separated by a selected distance. Crossover measurement points are defined by intersections of the horizontal and vertical rods. By selectively and sequentially applying a pulse to the vertical rods and concurrently biasing horizontal rods, measurements can be obtained for the crossover measurement points, which can then be employed to determine ion beam shape and ion beam intensity at the crossover measurement points. Based on these measurements, adjustments can be made to a continuing ion implantation process in order to increase uniformity with respect to intensity as well as to provide a desired beam shape. Additionally, pairs of vertical and horizontal rods can be employed to also obtain measurements that indicate angle of incidence in two dimensions at the various crossover points.
    • 本发明的离子束均匀性检测器包括多个水平杆和多个垂直杆,放置在平行平面上并分开一定距离。 交叉测量点由水平杆和垂直杆的交点定义。 通过选择性地并且顺序地向垂直杆施加脉冲并且同时偏置水平杆,可以获得交叉测量点的测量值,然后可以采用该测量点来确定交叉测量点处的离子束形状和离子束强度。 基于这些测量,可以进行连续离子注入工艺的调整,以便增加相对于强度的均匀性以及提供期望的光束形状。 此外,可以使用成对的垂直杆和水平杆来获得在各个交叉点处二维指示入射角的测量。
    • 34. 发明授权
    • Electrostatic parallelizing lens for ion beams
    • 离子束静电平行化透镜
    • US06774377B1
    • 2004-08-10
    • US10607239
    • 2003-06-26
    • Robert D. RathmellVictor M. Benveniste
    • Robert D. RathmellVictor M. Benveniste
    • H01J37317
    • H01J37/3171H01J37/12
    • A lens structure for use with an ion beam implanter. The lens structure includes first and second electrodes spaced apart along a direction of ion movement. The lens structure extends on opposite sides of a beam path across a width of the ion beam for deflecting ions entering the lens structure. The lens structure include a first electrode for decelerating ions and a second electrode for accelerating the ions to cause ions entering the lens structure to exit said lens structure with approximately the same exit trajectory regardless of the trajectory ions enter the lens structure. In an alternate construction the lens structure can include a first electrode for accelerating ions and a second electrode for decelerating ions.
    • 用于离子束注入机的透镜结构。 透镜结构包括沿离子运动方向间隔开的第一和第二电极。 透镜结构在离子束的宽度上的光束路径的相对侧上延伸,用于偏转进入透镜结构。 透镜结构包括用于减速离子的第一电极和用于加速离子的第二电极,使离子进入透镜结构以离开所述透镜结构以大致相同的出射轨迹,而与轨迹离子进入透镜结构无关。 在替代结构中,透镜结构可以包括用于加速离子的第一电极和用于减速离子的第二电极。
    • 37. 发明授权
    • Accelerator-decelerator electrostatic lens for variably focusing and
mass resolving an ion beam in an ion implanter
    • US5780863A
    • 1998-07-14
    • US841725
    • 1997-04-29
    • Victor M. BenvenistePeter L. Kellerman
    • Victor M. BenvenistePeter L. Kellerman
    • C23C14/48H01J37/12H01J37/30H01J37/317H01L21/265H01J37/10
    • H01J37/3171H01J37/3007H01J2237/047H01J2237/1207
    • An electrostatic triode lens (36) is provided for use in an ion implantation system (10). The lens includes a terminal electrode (37) and an adjustable lens subassembly (40) comprising a suppression electrode (38) and a resolving electrode (39), each having matched curved surfaces (108, 110). The lens subassembly is positioned near the terminal electrode where the beam has a minimal waist in a first (dispersive) plane. Such positioning minimizes the required gaps between electrodes, and thus, helps minimize beam blow-up and the electron depletion region in the deceleration mode of operation. The suppression and resolving electrodes each have first and second portions (38A and 38B, 39A and 39B) separated by a gap (d38, d39). A movement mechanism (60, 62) simultaneously moves the first portions of the suppression and resolving electrodes (38A, 39A) toward and away from the second portions of the suppression and resolving electrodes (38B, 39B), respectively, to adjust the gaps (d38, d39) therebetween. The adjustable lens subassembly (40) conditions the beam output by the terminal electrode (37) by (i) variably focusing the beam in mutually orthogonal (dispersive and non-dispersive) planes in a deceleration mode of operation (where mass resolution is less critical), while (ii) permitting variable mass resolution in the dispersive plane in an acceleration mode of operation (where focusing is less critical). Generally, the gap (d39) between the resolving electrode pair (39) is adjusted to permit adjustable mass resolution in the dispersive plane in the acceleration mode of operation. In the deceleration mode of operation, adjustment of the gap (d39) provides adjustable dispersive plane focusing, while the voltage on suppression electrode (38) is adjusted to permit adjustable non-dispersive plane beam focusing.