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    • 71. 发明授权
    • Objective with birefringent lenses
    • 目标双折射镜片
    • US06992834B2
    • 2006-01-31
    • US11071523
    • 2005-03-02
    • Michael TotzeckVladimer KamenovDaniel KraehmerWilhelm Ulrich
    • Michael TotzeckVladimer KamenovDaniel KraehmerWilhelm Ulrich
    • G02B21/02
    • G02B1/08G02B1/02G02B5/3083G02B13/143G03F7/70241G03F7/705G03F7/70966
    • Objective (1, 601), in particular a projection objective for a microlithography projection apparatus, with first birefringent lenses (L108, L109, L129, L130) and with second birefringent lenses (L101–L107, L110–L128). The first lenses (L108, L109, L129, L130) are distinguished from the second lenses (L101–L107, L110–L128) by the lens material used or by the material orientation. After passing through the first lenses (L108, L109, L129, L130) and the second lenses (L101–L107, L110–L128), an outer aperture ray (5, 7) and a principal ray (9) are subject to optical path differences for two mutually orthogonal states of polarization. The difference between these optical path differences is smaller than 25% of the working wavelength. In at least one first lens (L129, L130), the aperture angle of the outer aperture ray (5, 7) is at least 70% of the largest aperture angle occurring for said aperture ray in all of the first lenses (L108, L109, L129, L130) and second lenses (L101–L107, L110–L128). This arrangement has the result that the first lenses (L108, L109, L129, L130) have a combined material volume of no more than 20% of the combined total material volume of the first lenses (L108, L109, L129, L130) and second lenses (L101–L107, L110–L128).
    • 目的(1,601),特别是具有第一双折射透镜(L108,L109,L129,L130)和第二双折射透镜(L101-L107,L110-L128)的微光刻投影装置的投影物镜。 第一透镜(L108,L109,L129,L130)与所使用的透镜材料或材料取向与第二透镜(L101-L107,L110-L128)不同。 在通过第一透镜(L108,L109,L129,L130)和第二透镜(L101-L107,L110-L128)之后,外光线(5,7)和主光线(9)经受光路 两个相互正交的极化状态的差异。 这些光程差之差小于工作波长的25%。 在至少一个第一透镜(L129,L130)中,外光圈(5,7)的孔径角为所有第一透镜(L108,L109)中的所述孔径光线发生的最大孔径角的至少70% ,L129,L130)和第二透镜(L101-L107,L110-L128)。 这种结构的结果是,第一透镜(L108,L109,L129,L130)的组合材料体积不超过第一透镜(L108,L109,L129,L130)和第二透镜 镜头(L101-L107,L110-L128)。
    • 79. 发明申请
    • Imaging system for emulation of a high aperture scanning system
    • 用于高光圈扫描系统仿真的成像系统
    • US20060007541A1
    • 2006-01-12
    • US10923551
    • 2004-08-20
    • Michael TotzeckUlrich StroessnerJoern Greif-Wuestenbecker
    • Michael TotzeckUlrich StroessnerJoern Greif-Wuestenbecker
    • G02B5/30
    • G03F7/70566G02B21/002G02B27/286G03F7/70666
    • The present invention is directed to an optical imaging system for inspection microscopes with which lithography masks can be checked for defects particularly through emulation of high-aperture scanner systems. The imaging system, according to the invention, for emulating high-aperture scanner systems comprises imaging optics, a detector and an evaluating unit, wherein at least one polarization-active optical element is arranged as desired in the imaging beam path for selection of different polarization components of the imaging beam, an optical element with intensity attenuation function can be introduced in the imaging beam path, images of the mask and/or sample are received by the detector for differently polarized beam components and are conveyed to the evaluating unit for further processing. With the proposed solution, it is possible in particular to examine lithography masks for defects in spite of increasingly smaller structures and increasingly higher image-side numerical apertures of the imaging systems by means of inspection microscopes with high magnifications. Realistic images of the stepper systems can be generated by emulating the occurring vector effects.
    • 本发明涉及一种用于检查显微镜的光学成像系统,通过该光学成像系统可以通过光学掩模来检查缺陷,特别是通过高光阑扫描器系统的仿真。 根据本发明的用于模拟高光圈扫描器系统的成像系统包括成像光学器件,检测器和评估单元,其中至少一个偏振有源光学元件根据需要在成像光束路径中布置以选择不同的极化 成像光束的成分,具有强度衰减功能的光学元件可以被引入到成像光束路径中,掩模和/或样品的图像由检测器接收以用于不同偏振的光束分量,并被传送到评估单元进行进一步处理 。 利用所提出的解决方案,可以通过借助于具有高放大率的检查显微镜,检查光刻掩模的缺陷,尽管结构越来越小,成像系统的图像侧数值孔径越来越高。 可以通过仿真出现的矢量效应来生成步进系统的现实图像。
    • 80. 发明申请
    • Objective with birefringent lenses
    • 目标双折射镜片
    • US20050200966A1
    • 2005-09-15
    • US11071523
    • 2005-03-02
    • Michael TotzeckVladimer KamenovDaniel KraehmerWilhelm Ulrich
    • Michael TotzeckVladimer KamenovDaniel KraehmerWilhelm Ulrich
    • G02B1/02G02B5/30G02B13/14G02B13/18G03F7/20H01L21/027G02B3/00G02B9/00G02B15/14
    • G02B1/08G02B1/02G02B5/3083G02B13/143G03F7/70241G03F7/705G03F7/70966
    • Objective (1, 601), in particular a projection objective for a microlithography projection apparatus, with first birefringent lenses (L108, L109, L129, L130) and with second birefringent lenses (L101-L107, L110-L128). The first lenses (L108, L109, L129, L130) are distinguished from the second lenses (L101-L107, L110-L128) by the lens material used or by the material orientation. After passing through the first lenses (L108, L109, L129, L130) and the second lenses (L101-L107, L110-L128), an outer aperture ray (5, 7) and a principal ray (9) are subject to optical path differences for two mutually orthogonal states of polarization. The difference between these optical path differences is smaller than 25% of the working wavelength. In at least one first lens (L129, L130), the aperture angle of the outer aperture ray (5, 7) is at least 70% of the largest aperture angle occurring for said aperture ray in all of the first lenses (L108, L109, L129, L130) and second lenses (L101-L107, L110-L128). This arrangement has the result that the first lenses (L108, L109, L129, L130) have a combined material volume of no more than 20% of the combined total material volume of the first lenses (L108, L109, L129, L130) and second lenses (L101-L107, L110-L128).
    • 目的(1,601),特别是具有第一双折射透镜(L 108,L 109,L 129,L 130)和第二双折射透镜(L 101 -L 107,L 110-110)的微光刻投影装置的投影物镜, L 128)。 第一透镜(L 108,L 109,L 129,L 130)与所使用的透镜材料或材料取向与第二透镜(L 101 -L 107,L 110 -L 128)不同。 在穿过第一透镜(L 108,L 109,L 129,L 130)和第二透镜(L 101 -L 107,L 110 -L 128)之后,外孔光线(5,7)和主光线 (9)对于两个相互正交的极化状态经受光程差。 这些光程差之差小于工作波长的25%。 在至少一个第一透镜(L 129,L 130)中,外孔径光线(5,7)的孔径角度是所有第一透镜中的所述孔径光线发生的最大孔径角的至少70%(L 108,L 109,L 129,L 130)和第二透镜(L 101 -L 107,L 110 -L 128)。 这种结构的结果是,第一透镜(L 108,L 109,L 129,L 130)的组合材料体积不超过第一透镜(L 108,L 109,L 130, L 129,L 130)和第二透镜(L 101 -L 107,L 110 -L 128)。