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    • 7. 发明申请
    • Charged Particle Beam Device and Charged Particle Beam Measurement Method
    • 带电粒子束装置和带电粒子束测量方法
    • US20160225583A1
    • 2016-08-04
    • US15021039
    • 2014-05-30
    • HITACHI HIGH-TECHNOLOGIES CORPORATION
    • Natsuki TSUNOYoshinobu KIMURAHideyuki KAZUMIHajime KAWANOJunichiro TOMIZAWA
    • H01J37/28H01J37/244
    • H01J37/28H01J37/244H01J37/265H01J2237/043
    • 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.
    • 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。
    • 10. 发明申请
    • CHARGED PARTICLE BEAM APPLICATION DEVICE
    • 充电颗粒光束应用器件
    • US20150364290A1
    • 2015-12-17
    • US14741324
    • 2015-06-16
    • HITACHI HIGH-TECHNOLOGIES CORPORATION
    • Momoyo ENYAMAAkira IKEGAMIHideto DOHIHideyuki KAZUMINaomasa SUZUKI
    • H01J37/147H01J37/06H01J37/141
    • H01J37/1478H01J37/153H01J37/28H01J2237/1534
    • The charged particle beam application device is provided with a charged particle source and an objective lens that converges charged particle beam generated by the charged particle source onto a sample. In this case, the charged particle beam application device is further provided with an aberration generating element installed between the charged particle beam source and the objective lens, a tilt-use deflector installed between the aberration generating element and the objective lens, a deflection aberration control unit for controlling the aberration generating element, a first electromagnetic field superposing multipole installed between the aberration generating element and the objective lens, and an electromagnetic field superposing multipole control unit for controlling the first electromagnetic field superposing multipole. The aberration generating element has such a function that when the charged particle beam is tilted relative to the sample by the tilt-use deflector, a plurality of resulting aberrations are cancelled with one another. Moreover, the first electromagnetic field superposing multipole has a function to change the orbit of a charged particle beam having energy different from that of the main charged particle beam in the charged particle beam.
    • 带电粒子束施加装置设置有带电粒子源和将由带电粒子源产生的带电粒子束会聚到样本上的物镜。 在这种情况下,带电粒子束施加装置还设置有安装在带电粒子束源和物镜之间的像差产生元件,安装在像差产生元件和物镜之间的倾斜用偏转器,偏转像差控制 用于控制像差产生元件的单元,安装在像差产生元件和物镜之间的第一电磁场叠加多极,以及用于控制第一电磁场叠加多极的电磁场叠加多极控制单元。 像差产生元件具有这样的功能:当通过倾斜使用偏转器使带电粒子束相对于样本倾斜时,多个得到的像差彼此抵消。 此外,第一电磁场叠加多极具有改变具有与带电粒子束中的主带电粒子束的能量不同的能量的带电粒子束的轨道的功能。