METHOD OF MEASURING ASYMMETRY, INSPECTION APPARATUS, LITHOGRAPHIC SYSTEM AND DEVICE MANUFACTURING METHOD
    4.
    发明申请
    METHOD OF MEASURING ASYMMETRY, INSPECTION APPARATUS, LITHOGRAPHIC SYSTEM AND DEVICE MANUFACTURING METHOD 审中-公开
    测量不对称的方法,检查装置,光刻系统和器件制造方法

    公开(公告)号:WO2016096524A1

    公开(公告)日:2016-06-23

    申请号:PCT/EP2015/078915

    申请日:2015-12-08

    Abstract: A scatterometer is used in a dark-field imaging mode to measure asymmetry-related parameters such overlay. Measurements of small grating targets are made using identical optical paths, with the target in two orientations to obtain separate measurements of +1 and -1 diffraction orders. In this way, intensity scaling differences (tool asymmetry) are avoided. However, additive Intensity defects due to stray light (ghosts) in the optical system cannot be avoided. Additive intensity issues strongly depend on the ratio between 0th and 1st order diffraction and are therefore strongly wafer (process) dependent opposite. Calibration measurements (CM1-CM4) are made on a few representative target gratings having biases (+d, –d). The calibration measurements are made, using not only different wafer rotation (RZ = 0, π ) but also complementary apertures (13N, 13S). Corrections (δ, G) are calculated and applied calculate corrected asymmetry A', to reduce error caused by stray light.

    Abstract translation: 在暗场成像模式中使用散射仪来测量不对称相关参数,如覆盖。 使用相同的光路进行小光栅靶的测量,其中目标在两个取向中以获得+1和-1衍射级的单独测量。 以这种方式,避免了强度缩放差异(工具不对称)。 然而,由于光学系统中的杂散光(重影)引起的附加强度缺陷是无法避免的。 添加强度问题很大程度上取决于第0级和第1级衍射之间的比例,因此强晶片(工艺)依赖相反。 校准测量(CM1-CM4)在具有偏差(+ d,-d)的几个代表性目标光栅上进行。 进行校准测量,不仅使用不同的晶片旋转(RZ = 0,π),而且使用互补孔(13N,13S)。 校正(δ,G)被计算并应用计算校正不对称A',以减少由杂散光引起的误差。

    METHOD OF DETERMING A VALUE OF A PARAMETER OF INTEREST OF A PATTERNING PROCESS, DEVICE MANUFACTURING METHOD

    公开(公告)号:EP3647871A1

    公开(公告)日:2020-05-06

    申请号:EP18203837.2

    申请日:2018-10-31

    Abstract: The disclosure relates to determining a value of a parameter of interest of a patterning process. A plurality of calibration data units is obtained from targets in a metrology process. Each of at least two of the calibration data units represents detected radiation obtained using different respective polarization settings in the metrology process, each polarization setting defining a polarization property of incident radiation of the metrology process and a polarization property of detected radiation of the metrology process. The calibration data units are used to obtain calibration information about the metrology process. A measurement data unit representing detected radiation scattered from a further target is obtained, the further target comprising a structure formed using the patterning process on the substrate or on a further substrate. The value of the parameter of interest is determined using the measurement data unit and the obtained calibration information.

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