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    • 71. 发明授权
    • System for scatterometric measurements and applications
    • 散射测量和应用系统
    • US07821654B2
    • 2010-10-26
    • US12410379
    • 2009-03-24
    • Anatoly FabrikantGuoheng ZhaoDaniel C. WackMehrdad Nikoonahad
    • Anatoly FabrikantGuoheng ZhaoDaniel C. WackMehrdad Nikoonahad
    • G01B11/34G01J4/00
    • G01N21/45G01N21/21G01N21/4788G01N21/9501G01N2021/213G01N2021/217G01N2021/8416G02B5/18
    • Instead of constructing a full multi-dimensional look-up-table as a model to find the critical dimension or other parameters in scatterometry, regression or other optimized estimation methods are employed starting from a “best guess” value of the parameter. Eigenvalues of models that are precalculated may be stored and reused later for other structures having certain common characteristics to save time. The scatterometric data that is used to find the value of the one or more parameter can be limited to those at wavelengths that are less sensitive to the underlying film characteristics. A model for a three-dimensional grating may be constructed by slicing a representative structure into a stack of slabs and creating an array of rectangular blocks to approximate each slab. One dimensional boundary problems may be solved for each block which are then matched to find a two-dimensional solution for the slab. A three-dimensional solution can then be constructed from the two-dimensional solutions for the slabs to yield the diffraction efficiencies of the three-dimensional grating. This model can then be used for finding the one or more parameters of the diffracting structure in scatterometry. Line roughness of a surface can be measured by directing a polarized incident beam in an incident plane normal to the line grating and measuring the cross-polarization coefficient. The value of the one or more parameters may then be supplied to a stepper or etcher to adjust a lithographic or etching process.
    • 不需要构建一个完整的多维查找表作为模型来查找散点图中的关键维度或其他参数,而是从参数的“最佳猜测”值开始采用回归或其他优化的估计方法。 预先计算的模型的特征值可以稍后存储并重用于具有某些共同特征的其他结构以节省时间。 用于查找一个或多个参数的值的散点数据可以限于那些对底层薄膜特性较不敏感的波长数据。 三维光栅的模型可以通过将代表性结构切片成一叠平板并且产生矩形块阵列来近似每个平板来构造。 可以为每个块解决一维边界问题,然后将其匹配以找到板的二维解。 然后可以从板的二维解决方案中构建三维解,以产生三维光栅的衍射效率。 然后,该模型可用于在散射测量中找到衍射结构的一个或多个参数。 可以通过将垂直于线光栅的入射平面中的偏振入射光束引导并测量交叉极化系数来测量表面的线粗糙度。 然后可以将一个或多个参数的值提供给步进器或蚀刻器以调整光刻或蚀刻工艺。
    • 75. 发明授权
    • System for scatterometric measurements and applications
    • 散射测量和应用系统
    • US07301649B2
    • 2007-11-27
    • US11192056
    • 2005-07-27
    • Anatoly FabrikantGuoheng ZhaoDaniel C. WackMehrdad Nikoonahad
    • Anatoly FabrikantGuoheng ZhaoDaniel C. WackMehrdad Nikoonahad
    • G01B11/34G01J4/00
    • G01N21/45G01N21/21G01N21/4788G01N21/9501G01N2021/213G01N2021/217G01N2021/8416G02B5/18
    • Instead of constructing a full multi-dimensional look-up-table as a model to find the critical dimension or other parameters in scatterometry, regression or other optimized estimation methods are employed starting from a “best guess” value of the parameter. Eigenvalues of models that are precalculated may be stored and reused later for other structures having certain common characteristics to save time. The scatterometric data that is used to find the value of the one or more parameter can be limited to those at wavelengths that are less sensitive to the underlying film characteristics. A model for a three-dimensional grating may be constructed by slicing a representative structure into a stack of slabs and creating an array of rectangular blocks to approximate each slab. One dimensional boundary problems may be solved for each block which are then matched to find a two-dimensional solution for the slab. A three-dimensional solution can then be constructed from the two-dimensional solutions for the slabs to yield the diffraction efficiencies of the three-dimensional grating. This model can then be used for finding the one or more parameters of the diffracting structure in scatterometry. Line roughness of a surface can be measured by directing a polarized incident beam in an incident plane normal to the line grating and measuring the cross-polarization coefficient. The value of the one or more parameters may then be supplied to a stepper or etcher to adjust a lithographic or etching process.
    • 不需要构建一个完整的多维查找表作为模型来查找散点图中的关键维度或其他参数,而是从参数的“最佳猜测”值开始采用回归或其他优化的估计方法。 预先计算的模型的特征值可以稍后存储并重用于具有某些共同特征的其他结构以节省时间。 用于查找一个或多个参数的值的散点数据可以限于那些对底层薄膜特性较不敏感的波长数据。 三维光栅的模型可以通过将代表性结构切片成一叠平板并且产生矩形块阵列来近似每个平板来构造。 可以为每个块解决一维边界问题,然后将其匹配以找到板的二维解。 然后可以从板的二维解决方案中构建三维解,以产生三维光栅的衍射效率。 然后,该模型可用于在散射测量中找到衍射结构的一个或多个参数。 可以通过将垂直于线光栅的入射平面中的偏振入射光束引导并测量交叉极化系数来测量表面的线粗糙度。 然后可以将一个或多个参数的值提供给步进器或蚀刻器以调整光刻或蚀刻工艺。
    • 76. 发明授权
    • Method and system for improved defect sensitivity for inspecting surfaces
    • 提高检测表面缺陷灵敏度的方法和系统
    • US07221444B1
    • 2007-05-22
    • US11251129
    • 2005-10-14
    • Guoheng Zhao
    • Guoheng Zhao
    • G01N21/00
    • G01N21/9501G01N21/8806
    • Techniques for inspecting a substrate with improved defect sensitivity are disclosed. High sensitivity is achieved by reducing the noise due by using multiple laser beams for illumination, in which each beam is nearly collimated and illuminates uniformly a field of view. The images generated respectively by the laser beams are added incoherently by means of delivering the illumination beams incoherently in either time domain or space domain. According to one embodiment, all the illumination beams may not be interact with each other coherently so that the images generated by each laser beams can be summed together incoherently to average out possible excessive noise.
    • 公开了用于检查具有改善的缺陷灵敏度的衬底的技术。 通过减少使用多个激光束照明的噪音来实现高灵敏度,其中每个光束几乎被准直并且均匀地照射视场。 通过在时域或空域中不连续地传递照明光束,通过激光束分别产生的图像被非相干地添加。 根据一个实施例,所有照明光束可以不相干地相互作用,使得由每个激光束产生的图像可以非相干地相加在一起,以平均排除可能的过多噪声。
    • 79. 发明申请
    • System for scatterometric measurements and applications
    • 散射测量和应用系统
    • US20050274901A1
    • 2005-12-15
    • US11192056
    • 2005-07-27
    • Anatoly FabrikantGuoheng ZhaoDaniel WackMehrdad Nikoonahad
    • Anatoly FabrikantGuoheng ZhaoDaniel WackMehrdad Nikoonahad
    • G01B11/00G01B11/30G01N21/21G01N21/27G01N21/47G01N21/95G02B5/18G03F1/08H01L21/027H01L21/66G06F19/00
    • G01N21/45G01N21/21G01N21/4788G01N21/9501G01N2021/213G01N2021/217G01N2021/8416G02B5/18
    • Instead of constructing a full multi-dimensional look-up-table as a model to find the critical dimension or other parameters in scatterometry, regression or other optimized estimation methods are employed starting from a “best guess” value of the parameter. Eigenvalues of models that are precalculated may be stored and reused later for other structures having certain common characteristics to save time. The scatterometric data that is used to find the value of the one or more parameter can be limited to those at wavelengths that are less sensitive to the underlying film characteristics. A model for a three-dimensional grating may be constructed by slicing a representative structure into a stack of slabs and creating an array of rectangular blocks to approximate each slab. One dimensional boundary problems may be solved for each block which are then matched to find a two-dimensional solution for the slab. A three-dimensional solution can then be constructed from the two-dimensional solutions for the slabs to yield the diffraction efficiencies of the three-dimensional grating. This model can then be used for finding the one or more parameters of the diffracting structure in scatterometry. Line roughness of a surface can be measured by directing a polarized incident beam in an incident plane normal to the line grating and measuring the cross-polarization coefficient. The value of the one or more parameters may then be supplied to a stepper or etcher to adjust a lithographic or etching process.
    • 不需要构建一个完整的多维查找表作为模型来查找散点图中的关键维度或其他参数,而是从参数的“最佳猜测”值开始采用回归或其他优化的估计方法。 预先计算的模型的特征值可以稍后存储并重用于具有某些共同特征的其他结构以节省时间。 用于查找一个或多个参数的值的散点数据可以限于那些对底层薄膜特性较不敏感的波长数据。 三维光栅的模型可以通过将代表性结构切片成一叠平板并且产生矩形块阵列来近似每个平板来构造。 可以为每个块解决一维边界问题,然后将其匹配以找到板的二维解。 然后可以从板的二维解决方案中构建三维解,以产生三维光栅的衍射效率。 然后,该模型可用于在散射测量中找到衍射结构的一个或多个参数。 可以通过将垂直于线光栅的入射平面中的偏振入射光束引导并测量交叉极化系数来测量表面的线粗糙度。 然后可以将一个或多个参数的值提供给步进器或蚀刻器以调整光刻或蚀刻工艺。
    • 80. 发明申请
    • System for measuring periodic structures
    • US20050099627A1
    • 2005-05-12
    • US11016148
    • 2004-12-17
    • Guoheng ZhaoKenneth GrossRodney SmedtMehrdad Nikoonahad
    • Guoheng ZhaoKenneth GrossRodney SmedtMehrdad Nikoonahad
    • G01B11/00G01J4/00
    • G01N21/21G01B11/00G01N21/4788G01N21/956
    • A periodic structure is illuminated by polychromatic electromagnetic radiation. Radiation from the structure is collected and divided into two rays having different polarization states. The two rays are detected from which one or more parameters of the periodic structure may be derived. In another embodiment, when the periodic structure is illuminated by a poly chromatic electromagnetic radiation, the collected radiation from the structure is passed through a polarization element having a polarization plane. The element and the polychromatic beam are controlled so that the polarization plane of the element are at two or more different orientations with respect to the plane of incidence of the polychromatic beam. Radiation that has passed through the element is detected when the plane of polarization is at the two or more positions so that one or more parameters of the periodic structure may be derived from the detected signals. At least one of the orientations of the plane of polarization is substantially stationary when the detection takes place. To have as small a footprint as possible, one employs an optical device that includes a first element directing a polychromatic beam of electromagnetic radiation to the structure and a second optical element collecting radiation from the structure where the two elements form an integral unit or are attached together to form an integrated unit. To reduce the footprint, the measurement instrument and the wafer are both moved. In one embodiment, both the apparatus and the wafer undergo translational motion transverse to each other. In a different arrangement, one of the two motions is translational and the other is rotational. Any one of the above-described embodiments may be included in an integrated processing and detection apparatus which also includes a processing system processing the sample, where the processing system is responsive to the output of any one of the above embodiments for adjusting a processing parameter.