Charged particle beam device and arithmetic device
    1.
    发明授权
    Charged particle beam device and arithmetic device 有权
    带电粒子束装置和运算装置

    公开(公告)号:US09530614B2

    公开(公告)日:2016-12-27

    申请号:US14373123

    申请日:2012-12-17

    Abstract: It is possible to determine an optimal parasitic aberration adjustment amount even when the relationship of the parasitic aberration adjustment amount with respect to the field intensity of multiple poles changes nonlinearly. To this end, in the present invention, an aberration correction amount is computed by measuring an aberration coefficient of an optical unit of a charged particle beam device, and at the same time, the present value of a power supply control value applied to an aberration corrector is measured. Then, the parasitic aberration adjustment amount for suppressing the amount of a parasitic aberration generated in the aberration corrector is computed on the basis of the aberration correction amount and the present value of the power supply control value.

    Abstract translation: 即使当寄生像差调整量相对于多个磁场强度的关系非线性地变化时,也可以确定最佳的寄生像差调整量。 为此,在本发明中,通过测量带电粒子束装置的光学单元的像差系数来计算像差校正量,同时,应用于像差的电源控制值的当前值 校正器被测量。 然后,基于像差校正量和电源控制值的当前值来计算用于抑制像差校正器中产生的寄生像差量的寄生像差调整量。

    CHARGED PARTICLE BEAM DEVICE AND ARITHMETIC DEVICE
    3.
    发明申请
    CHARGED PARTICLE BEAM DEVICE AND ARITHMETIC DEVICE 有权
    充电颗粒光束装置和算术装置

    公开(公告)号:US20150060654A1

    公开(公告)日:2015-03-05

    申请号:US14373123

    申请日:2012-12-17

    Abstract: It is possible to determine an optimal parasitic aberration adjustment amount even when the relationship of the parasitic aberration adjustment amount with respect to the field intensity of multiple poles changes nonlinearly. To this end, in the present invention, an aberration correction amount is computed by measuring an aberration coefficient of an optical unit of a charged particle beam device, and at the same time, the present value of a power supply control value applied to an aberration corrector is measured. Then, the parasitic aberration adjustment amount for suppressing the amount of a parasitic aberration generated in the aberration corrector is computed on the basis of the aberration correction amount and the present value of the power supply control value.

    Abstract translation: 即使当寄生像差调整量相对于多个磁场强度的关系非线性地变化时,也可以确定最佳的寄生像差调整量。 为此,在本发明中,通过测量带电粒子束装置的光学单元的像差系数来计算像差校正量,同时,应用于像差的电源控制值的当前值 校正器被测量。 然后,基于像差校正量和电源控制值的当前值来计算用于抑制像差校正器中产生的寄生像差量的寄生像差调整量。

    MULTIPOLE MEASUREMENT APPARATUS
    5.
    发明申请
    MULTIPOLE MEASUREMENT APPARATUS 有权
    多点测量装置

    公开(公告)号:US20140217304A1

    公开(公告)日:2014-08-07

    申请号:US14241035

    申请日:2012-05-23

    Abstract: In order to provide a multipole measurement apparatus that can easily obtain table data for an aberration corrector that corrects the aberrations in a charged particle beam apparatus, the multipole measurement apparatus, which is provided with an optical system (10), a space into which an aberration corrector (6) is to be inserted, and a position detector (7), measures the relationship between the incident position and angle of a primary charged particle beam on the aberration corrector (6) at a plurality of points, the irradiation position upon the position detector (7), and a multipole, in a state of having a multipole field excited and in a state of not having a multipole field excited, so as to extract multipole components contained in the measurement executed in the state of having the multipole field excited.

    Abstract translation: 为了提供一种可以容易地获得用于校正带电粒子束装置中的像差的像差校正器的表格数据的多极测量装置,具有光学系统(10)的多极测量装置, 将像差校正器(6)插入,并且位置检测器(7)测量多个点处的像差校正器(6)上的初级带电粒子束的入射位置和角度之间的关系, 位置检测器(7)和多极,具有被激励的多极场的状态,并且处于不具有多极场激励的状态,以便提取包含在具有多极的状态下的测量中的多极分量 场激动

    Charged particle beam device and aberration correction method for charged particle beam device

    公开(公告)号:US10727024B2

    公开(公告)日:2020-07-28

    申请号:US16325613

    申请日:2016-08-23

    Abstract: A charged particle beam device using a multi-pole type aberration corrector includes: a charged particle source which generates a primary charged particle beam; an aberration correction optical system which corrects aberrations of the primary charged particle beam; a detection unit which detects a secondary charged particle generated from a sample irradiated with the primary charged particle beam whose aberrations have been corrected; an image forming unit which forms a charged particle image of the sample from a signal obtained by detecting the secondary charged particle; an aberration correction amount calculation unit which processes the charged particle image, separates aberrations having different symmetries, selects an aberration to be preferentially corrected from the separated aberrations, and calculates a correction amount of the aberration correction optical system; and an aberration correction optical system control unit which controls the aberration correction optical system based on the calculated correction amount.

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