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Method for determining a structure-independent contribution of a lithography mask to a fluctuation of the line width

机译:确定光刻掩模对线宽波动的与结构无关的贡献的方法

摘要

Method for determining a structure-independent contribution of a lithography mask (5) to a linewidth fluctuation (LWR) comprising the following steps: 1.1. Providing an optical system (2) with imaging optics (8) for imaging lithographic masks (5) 1.2. Providing a lithography mask (5) with at least one measuring range which is free of structures to be imaged, 1.3. Illuminating the at least one measuring range with illumination radiation (1), 1.4. Picking up a focus stack of the at least one measurement region of the lithography mask (5), 1.5. spatially resolved evaluation of 2D intensity distributions (15) of the recorded focus stack, wherein the evaluation of the 2D intensity distributions (15) comprises the following steps: 1.6. Determining a spectrum of the 2D intensity distributions (15) by Fourier transforming the 2D intensity distributions (15zi), 1.7. Determining a defocus dependence of a plurality of spectral components S (v, v) of the spectrum1.8. Determining a Fourier transform of a function to describe the optical surface roughness of the lithography mask (5) from the determined defocus dependence of the spectral components S (v, v), 1.9. wherein evaluating the 2D intensity distributions (15) comprises determining a speckle contrast (ΔI).
机译:确定光刻掩模(5)对线宽波动(LWR)的与结构无关的贡献的方法,包括以下步骤:1.1。提供具有用于成像光刻掩模(5)的成像光学器件(8)的光学系统(2)1.2。提供具有至少一个测量范围的光刻掩模(5),该测量范围没有要成像的结构,1.3。用照明辐射(1)1.4照明至少一个测量范围。拾取光刻掩模(5)的至少一个测量区域的聚焦叠层1.5。对记录的焦点堆栈的2D强度分布(15)进行空间分辨评估,其中对2D强度分布(15)进行评估包括以下步骤:1.6。通过傅立叶变换1.7的2D强度分布(15zi)确定2D强度分布(15)的光谱。确定光谱1.8的多个光谱分量S(v,v)的散焦依赖性。根据所确定的光谱分量S(v,v),1.9的散焦依赖性,确定用于描述光刻掩模(5)的光学表面粗糙度的函数的傅立叶变换。其中评估2D强度分布(15)包括确定斑点对比度(ΔI)。

著录项

  • 公开/公告号DE102018202639B4

    专利类型

  • 公开/公告日2019-11-21

    原文格式PDF

  • 申请/专利权人 CARL ZEISS SMT GMBH;

    申请/专利号DE201810202639

  • 申请日2018-02-21

  • 分类号G01M11/02;G03F7/20;G03F1/84;G01B11/24;G01B11/30;

  • 国家 DE

  • 入库时间 2022-08-21 11:01:44

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