Scanning microscope
    93.
    发明授权
    Scanning microscope 失效
    扫描显微镜

    公开(公告)号:US5929439A

    公开(公告)日:1999-07-27

    申请号:US868650

    申请日:1997-06-04

    CPC classification number: H01J37/28 G02B21/002 H01J2237/043 H01J2237/22

    Abstract: A scanned image to be observed or to be recorded is formed by a plurality of two-dimensional scanning times (N times), an irradiating charged particle beam or a light beam is blanked in a two-dimensional scanning unit, and the averaged irradiation intensity is adjusted by thinning a plurality (

    Abstract translation: 通过多次二维扫描时间(N次)形成待观察或待记录的扫描图像,照射带电粒子束或光束在二维扫描单元中被消隐,并且平均的照射强度 通过在N次扫描中减少多个(

    Single ion implantation system
    94.
    发明授权
    Single ion implantation system 失效
    单离子注入系统

    公开(公告)号:US5539203A

    公开(公告)日:1996-07-23

    申请号:US233513

    申请日:1994-04-26

    Applicant: Iwao Ohdomari

    Inventor: Iwao Ohdomari

    Abstract: The present invention is directed to a low-energy (0 to 100 keV) or high-energy (1 to 4 MeV) single ion implantation system in which single ions are extracted from a focused ion beam or micro-ion beam by beam chopping. The low-energy single ion implantation system has, in combination with a focused ion beam system, an electrostatic deflector for beam chopping (20), an aperture for single ion extraction (21) and an electrode (35) for generating a retarding electric field to make the single ion soft-land on a specimen. The high-energy single ion implantation system has, in combination with an ion microprobe, a Cs sputter source (33) which enables dopant ion implantation and high LET ion irradiation. The single ion implantation method includes a step of implanting the extracted single ions from the both systems into the specimen at a predetermined target position with aiming accuracies of 50 nm.phi. and 1.5 .mu.m.phi., respectively.

    Abstract translation: 本发明涉及一种低能量(0至100keV)或高能量(1至4MeV)单离子注入系统,其中通过束切割从聚焦离子束或微离子束中提取单个离子。 低能量单离子注入系统与聚焦离子束系统结合,用于束切割(20)的静电偏转器,用于单离子提取的孔(21)和用于产生延迟电场的电极(35) 使单个离子软土在样品上。 高能单离子注入系统与离子微探针组合具有能够进行掺杂剂离子注入和高LET离子照射的Cs溅射源(33)。 单离子注入方法包括分别将来自两个系统的提取的单个离子注入到预定目标位置的样品中的步骤,其瞄准精度分别为50nm phi和1.5μmphi。

    Ion irradiation system and method
    95.
    发明授权
    Ion irradiation system and method 失效
    离子照射系统及方法

    公开(公告)号:US5331161A

    公开(公告)日:1994-07-19

    申请号:US938611

    申请日:1992-09-01

    CPC classification number: H01J37/265 H01J37/28 H01J2237/043

    Abstract: The present invention concerns an ion irradiation system and has for its object to provide an ion irradiation system and method which enable one or more ions to be applied to a target point with high accuracy. The ion irradiation system according to the present invention comprises: an ion microprobe; a deflector for deflecting an ion microbeam generated by said ion microprobe; a micro slit for extracting a single or predetermined number of ions from said ion microbeam deflected by said deflector; a sample holder mechanism for holding a sample to be irradiated with said single or predetermined number of ions extracted through said micro slit; a scanning electron microscope mechanism for observing the surface of said sample in real time; a secondary electron detecting system for detecting secondary electrons which are emitted from the surface of said sample, said secondary electron detecting system including a secondary electron multiplier; and an electric field control circuit for controlling an electric field which is applied to said deflector, said electric field control circuit being composed of a clock generator, a counter connected to said clock generator and a high-voltage amplifier connected to said counter and having its output connected to said deflector; wherein said counter counts output signal pulses from said secondary electron multiplier and supplies a clock signal to said high-voltage amplifier of said electric field control circuit during counting of said single or predetermined number of ions and stops the supply of said clock signal to said high-voltage amplifier upon completion of counting of said single or predetermined number of ions, whereby said ion microbeam is chopped by said deflector one or more times instantaneously reverse its direction or deflection with respect to said micro slit, thereby extracting said single or predetermined number of ions through said micro slit.

    Abstract translation: 本发明涉及一种离子照射系统,其目的是提供一种能够以高精度将一个或多个离子施加到目标点的离子照射系统和方法。 根据本发明的离子辐射系统包括:离子微探针; 偏转器,用于偏转由所述离子微探针产生的离子微束; 用于从由所述偏转器偏转的所述离子微束中提取单个或预定数量的离子的微缝; 用于保持要通过所述微狭缝提取的所述单个或预定数量离子照射的样品的样品保持器机构; 用于实时观察所述样品表面的扫描电子显微镜机构; 用于检测从所述样品的表面发射的二次电子的二次电子检测系统,所述二次电子检测系统包括二次电子倍增器; 以及用于控制施加到所述偏转器的电场的电场控制电路,所述电场控制电路由时钟发生器,连接到所述时钟发生器的计数器和连接到所述计数器的高压放大器组成,并且具有其 输出连接到所述偏转器; 其中所述计数器对来自所述二次电子倍增器的输出信号脉冲进行计数,并且在所述单个或预定数量的离子计数期间将时钟信号提供给所述电场控制电路的所述高压放大器,并停止将所述时钟信号提供给所述高电平 在完成所述单个或预定数量的离子的计数之后,所述离子微束被所述偏转器斩波一次或多次,相对于所述微缝隙瞬时地反向其方向或偏转,从而提取所述单个或预定数量的 离子通过所述微缝隙。

    Method of and device for corpuscular projection
    96.
    发明授权
    Method of and device for corpuscular projection 失效
    粒子投影的方法和装置

    公开(公告)号:US4472636A

    公开(公告)日:1984-09-18

    申请号:US202046

    申请日:1980-10-30

    Applicant: Eberhard Hahn

    Inventor: Eberhard Hahn

    Abstract: The invention relates to a method of and device for producing any desired patterns on a target. The irradiating beam is modulated over the entire cross-sectional area by an electro-magnetic field, which is obtained by a line or two-dimensionally shaped electrode grid, each individual electrode of which can be differently charged and which reflects the irradiation beam or produces a respective strip.

    Abstract translation: 本发明涉及一种用于在目标上产生任何所需图案的方法和装置。 照射光束通过电磁场在整个横截面积上进行调制,该电磁场通过线或二维形状的电极栅格获得,每个电极栅格的每个单独电极可以被不同地充电并且反射照射束或产生 相应的条。

    Charged particle beam drawing apparatus and charged particle beam drawing method

    公开(公告)号:US09812284B2

    公开(公告)日:2017-11-07

    申请号:US15070679

    申请日:2016-03-15

    Inventor: Hideki Matsui

    Abstract: In one embodiment, a charged particle beam drawing apparatus deflects a charged particle beam with a deflector to draw a pattern. The apparatus includes a storage unit that stores an approximate formula indicating a correspondence relationship between a settling time for a DAC amplifier that controls the deflector, and a position shift amount, from a design position, of a drawn position of each evaluation pattern drawn on a first substrate while the settling time and an amount of deflection by the deflector are changed, a shot position correction unit that creates a correction formula indicating a relationship between an amount of deflection and a shot position shift amount at the settling time, from the approximate formula and the settling time for the DAC amplifier based on an amount of deflection of a shot, obtains a position correction amount by using the amount of deflection of the shot and the correction formula, and corrects a shot position defined by the shot data based on the position correction amount, and a drawing unit that performs drawing by using the shot data with a corrected shot position.

    Charged Particle Beam Device and Charged Particle Beam Measurement Method
    100.
    发明申请
    Charged Particle Beam Device and Charged Particle Beam Measurement Method 审中-公开
    带电粒子束装置和带电粒子束测量方法

    公开(公告)号:US20160225583A1

    公开(公告)日:2016-08-04

    申请号:US15021039

    申请日:2014-05-30

    CPC classification number: H01J37/28 H01J37/244 H01J37/265 H01J2237/043

    Abstract: An object of the present invention is to realize both of the accuracy of measuring the amount of secondary electron emissions and the stability of a charged particle beam image in a charged particle beam device. In a charged particle beam device, extraction of detected signals is started by a first trigger signal, the extraction of the detected signals is completed by a second trigger signal, the detected signals are sampled N times using N (N is a natural number) third trigger signals that equally divide an interval time T between the first trigger signal and the second trigger signal, secondary charged particles are measured by integrating and averaging the signals sampled in respective division times ΔT obtained by equally dividing the interval time T, and the division time ΔT is controlled in such a manner that the measured number of secondary charged particles becomes larger than the minimum number of charged particles satisfying ergodicity.

    Abstract translation: 本发明的目的在于实现测量二次电子发射量的精度和带电粒子束装置中的带电粒子束图像的稳定性。 在带电粒子束装置中,通过第一触发信号开始检测到的信号的提取,通过第二触发信号完成检测信号的提取,使用N(N是自然数)第三 触发信号,将第一触发信号和第二触发信号之间的间隔时间T均等地分开,通过对通过等分间隔时间T获得的各个分割时间ΔT中采样的信号进行积分和平均来测量次级带电粒子, 以这样的方式控制ΔT,使得测量的二次带电粒子的数量变得大于满足遍遍性的带电粒子的最小数量。

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