ELECTRON BEAM APPARATUS
    41.
    发明申请
    ELECTRON BEAM APPARATUS 有权
    电子束设备

    公开(公告)号:US20100102227A1

    公开(公告)日:2010-04-29

    申请号:US12257304

    申请日:2008-10-23

    Abstract: The present invention relates to a charged particle beam apparatus which employs a scanning electron microscope for sample inspection and defect review.The present invent provides solution of improving imaging resolution by utilizing a field emission cathode tip with a large tip radius, applying a large accelerating voltage across ground potential between the cathode and anode, positioning the beam limit aperture before condenser lens, utilizing condenser lens excitation current to optimize image resolution, applying a high tube bias to shorten electron travel time, adopting and modifying SORIL objective lens to ameliorate aberration at large field of view and under electric drifting and reduce the urgency of water cooling objective lens while operating material analysis.The present invent provides solution of improving throughput by utilizing fast scanning ability of SORIL and providing a large voltage difference between sample and detectors.

    Abstract translation: 本发明涉及采用扫描电子显微镜进行样品检查和缺陷检查的带电粒子束装置。 本发明提供了通过利用具有大的尖端半径的场致发射阴极尖端来提高成像分辨率的解决方案,在阴极和阳极之间的地电位上施加大的加速电压,将光束极限孔定位在聚光透镜之前,利用聚光透镜激发电流 优化图像分辨率,应用高管偏压缩短电子行进时间,采用和修正SORIL物镜,以改善大视野和电漂移下的像差,并减少水冷物镜在操作材料分析时的紧迫性。 本发明提供了通过利用SORIL的快速扫描能力并在样品和检测器之间提供大的电压差来提高产量的解决方案。

    Method and device for the regulation of a magnetic deflection system
    43.
    发明授权
    Method and device for the regulation of a magnetic deflection system 失效
    用于调节磁偏转系统的方法和装置

    公开(公告)号:US4380703A

    公开(公告)日:1983-04-19

    申请号:US183946

    申请日:1980-09-04

    Inventor: Reinhold Schmitt

    CPC classification number: H03K6/02 H01J37/24

    Abstract: In an exemplary embodiment, a command value signal is supplied to a magnetic deflection control loop which operates based on measurement of deflection coil current. A signal proportional to the rate of change of deflection magnetic field is supplied to one input of a differential amplifier, and a signal in accordance with the rate of change of the command value signal is connected with a second input of the differential amplifier. Any error between the rate of change signals as sensed by the differential amplifier is used as an auxiliary control of the deflection magnetic field, whereby eddy current influences are overcome. The system is particularly useful for precision control of an electron beam writer in the manufacture of semiconductor integrated circuits.

    Abstract translation: 在示例性实施例中,指令值信号被提供给基于偏转线圈电流的测量而工作的磁偏转控制回路。 与偏转磁场的变化率成比例的信号被提供给差分放大器的一个输入,并且根据指令值信号的变化率的信号与差分放大器的第二输入端相连。 由差分放大器感测到的变化率信号之间的任何误差被用作偏转磁场的辅助控制,从而克服了涡流影响。 该系统在半导体集成电路的制造中对电子束写入器的精确控制特别有用。

    CHARGED PARTICLE SOURCE
    47.
    发明申请

    公开(公告)号:US20220068589A1

    公开(公告)日:2022-03-03

    申请号:US17383353

    申请日:2021-07-22

    Inventor: Shuai LI

    Abstract: This invention provides a charged particle source, which comprises an emitter and means fo generating a magnetic field distribution. The magnetic field distribution is minimum, about zero, or preferred zero at the tip of the emitter, and along the optical axis is maximum away from the tip immediately. In a preferred embodiment, the magnetic field distribution is provided by dual magnetic lens which provides an anti-symmetric magnetic field at the tip, such that magnetic field at the tip is zero.

    Charged particle source
    48.
    发明授权

    公开(公告)号:US10468227B2

    公开(公告)日:2019-11-05

    申请号:US16042871

    申请日:2018-07-23

    Inventor: Shuai Li

    Abstract: This invention provides a charged particle source, which comprises an emitter and means of generating a magnetic field distribution. The magnetic field distribution is minimum, about zero, or preferred zero at the tip of the emitter, and along the optical axis is maximum away from the tip immediately. In a preferred embodiment, the magnetic field distribution is provided by dual magnetic lens which provides an anti-symmetric magnetic field at the tip, such that magnetic field at the tip is zero.

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