Illuminating a specimen for metrology or inspection
    62.
    发明授权
    Illuminating a specimen for metrology or inspection 有权
    照亮样本进行计量或检查

    公开(公告)号:US09080991B2

    公开(公告)日:2015-07-14

    申请号:US13073986

    申请日:2011-03-28

    IPC分类号: G01N21/00 G01N21/95 G01N21/47

    CPC分类号: G01N21/9501 G01N2021/479

    摘要: Illumination subsystems of a metrology or inspection system, metrology systems, inspection systems, and methods for illuminating a specimen for metrology measurements or for inspection are provided. One illumination subsystem includes a light source configured to generate coherent pulses of light and a dispersive element positioned in the path of the coherent pulses of light, which is configured to reduce coherence of the pulses of light by mixing spatial and temporal characteristics of light distribution in the pulses of light. The illumination subsystem also includes an electro-optic modulator positioned in the path of the pulses of light exiting the dispersive element and which is configured to reduce the coherence of the pulses of light by temporally modulating the light distribution in the pulses of light. The illumination subsystem is configured to direct the pulses of light from the electro-optic modulator to a specimen.

    摘要翻译: 提供了计量或检查系统的照明子系统,计量系统,检查系统和用于计量测量或检查的照明样本的方法。 一个照明子系统包括被配置为产生相干的光脉冲的光源和位于相干脉冲光的路径中的色散元件,该色散元件被配置为通过将光分布的空间和时间特征混合在一起来减小光脉冲的相干性 光的脉冲。 照明子系统还包括位于离开色散元件的光的脉冲的路径中的电光调制器,其被配置为通过暂时调制光脉冲中的光分布来减小光脉冲的相干性。 照明子系统被配置为将来自电光调制器的光脉冲引导到样本。

    Time-Resolved Single-Photon or Ultra-Weak Light Multi-Dimensional Imaging Spectrum System and Method
    63.
    发明申请
    Time-Resolved Single-Photon or Ultra-Weak Light Multi-Dimensional Imaging Spectrum System and Method 有权
    时间解决的单光子或超弱光多维成像光谱系统和方法

    公开(公告)号:US20140253713A1

    公开(公告)日:2014-09-11

    申请号:US14351028

    申请日:2012-05-14

    IPC分类号: G01N21/25 G01N21/64 G01N21/17

    摘要: A single-photon or ultra-weak light multi-D imaging spectral system and method. In order to realize rough time resolution, a time-resolved single-photon counting 2D imaging system for forming color or grey imaging is provided. Moreover, in order to realize high-precision time resolution, the system comprises a light source, an imaging spectral measurement unit, an electric detection unit, a system control unit and an algorithm unit. The light carrying information of an object is imaged on a spatial light modulator and randomly modulated according to compressed sensing theory, emergent light of a grating is collected using a point or array single-photon detector, the number of photons and photon arrival time are recorded, and reconstruction is carried out using the compressed sensing algorithm and related algorithm of the spectral imaging. The system provides single-photon detection sensitivity, high time resolution and wide spectral range, and can be applied in numerous new high-tech industries.

    摘要翻译: 单光子或超弱光多D成像光谱系统及方法。 为了实现粗糙的时间分辨率,提供了用于形成彩色或灰度成像的时间分辨的单光子计数2D成像系统。 此外,为了实现高精度时间分辨率,该系统包括光源,成像光谱测量单元,电检测单元,系统控制单元和算法单元。 物体的光携带信息在空间光调制器上成像,并且根据压缩感测理论随机调制,使用点或阵列单光子检测器收集光栅的出射光,记录光子数和光子到达时间 ,并利用压缩感知算法和相关的光谱成像算法进行重建。 该系统提供单光子检测灵敏度高,时间分辨率高,光谱范围广,可应用于众多新兴高科技行业。

    METHOD OF ELECTROMAGNETIC MODELING OF FINITE STRUCTURES AND FINITE ILLUMINATION FOR METROLOGY AND INSPECTION
    64.
    发明申请
    METHOD OF ELECTROMAGNETIC MODELING OF FINITE STRUCTURES AND FINITE ILLUMINATION FOR METROLOGY AND INSPECTION 有权
    有限结构的电磁建模方法和有限的照明方法和方法

    公开(公告)号:US20140222380A1

    公开(公告)日:2014-08-07

    申请号:US14170150

    申请日:2014-01-31

    IPC分类号: G01N21/27

    摘要: Electromagnetic modeling of finite structures and finite illumination for metrology and inspection are described herein. In one embodiment, a method for evaluating a diffracting structure involves providing a model of the diffracting structure. The method involves computing background electric or magnetic fields of an environment of the diffracting structure. The method involves computing scattered electric or magnetic fields from the diffracting structure using a scattered field formulation based on the computed background fields. The method further involves computing spectral information for the model of the diffracting structure based on the computed scattered fields, and comparing the computed spectral information for the model with measured spectral information for the diffracting structure. In response to a good model fit, the method involves determining a physical characteristic of the diffracting structure based on the model of the diffracting structure.

    摘要翻译: 本文描述了用于计量和检验的有限结构和有限照明的电磁建模。 在一个实施例中,用于评估衍射结构的方法包括提供衍射结构的模型。 该方法涉及计算衍射结构环境的背景电场或磁场。 该方法涉及使用基于所计算的背景场的散射场拟合来计算衍射结构中的散射电场或磁场。 该方法还涉及基于计算的散射场计算衍射结构模型的光谱信息,并将所计算的模型光谱信息与用于衍射结构的测量光谱信息进行比较。 响应于良好的模型拟合,该方法包括基于衍射结构的模型确定衍射结构的物理特性。

    Asymmetric wedge JFET, related method and design structure
    65.
    发明授权
    Asymmetric wedge JFET, related method and design structure 有权
    非对称楔形JFET,相关方法和设计结构

    公开(公告)号:US08481380B2

    公开(公告)日:2013-07-09

    申请号:US12888828

    申请日:2010-09-23

    IPC分类号: H01L21/337

    摘要: A junction gate field-effect transistor (JFET) for an integrated circuit (IC) chip is provided comprising a source region, a drain region, a lower gate, and a channel, with an insulating shallow trench isolation (STI) region extending from an inner edge of an upper surface of the source region to an inner edge of an upper surface of the drain region, without an intentionally doped region, e.g., an upper gate, coplanar with an upper surface of the IC chip between the source/drain regions. In addition, an asymmetrical quasi-buried upper gate can be included, disposed under a portion of the STI region, but not extending under a portion of the STI region proximate to the drain region. Embodiments of this invention also include providing an implantation layer, under the source region, to reduce Ron. A related method and design structure are also disclosed.

    摘要翻译: 提供了一种用于集成电路(IC)芯片的结栅场效应晶体管(JFET),其包括源极区,漏极区,下栅极和沟道,其中绝缘浅沟槽隔离(STI)区域从 源区域的上表面的内边缘到漏极区域的上表面的内边缘,而没有有意掺杂的区域,例如上栅极,与源极/漏极区域之间的IC芯片的上表面共面 。 此外,可以包括设置在STI区域的一部分下方的不对称的准掩埋的上栅极,但不在靠近漏极区域的STI区域的一部分下方延伸。 本发明的实施例还包括在源极区域下提供注入层以减少Ron。 还公开了相关的方法和设计结构。

    SEMICONDUCTOR STRUCTURE INCLUDING A HIGH PERFORMANCE FET AND A HIGH VOLTAGE FET ON AN SOI SUBSTRATE
    67.
    发明申请
    SEMICONDUCTOR STRUCTURE INCLUDING A HIGH PERFORMANCE FET AND A HIGH VOLTAGE FET ON AN SOI SUBSTRATE 有权
    在SOI衬底上包括高性能FET和高电压FET的半导体结构

    公开(公告)号:US20120132992A1

    公开(公告)日:2012-05-31

    申请号:US13367646

    申请日:2012-02-07

    IPC分类号: H01L27/12

    摘要: A first field effect transistor includes a gate dielectric and a gate electrode located over a first portion of a top semiconductor layer in a semiconductor-on-insulator (SOI) substrate. A second field effect transistor includes a portion of a buried insulator layer and a source region and a drain region located underneath the buried insulator layer. In one embodiment, the gate electrode of the second field effect transistor is a remaining portion of the top semiconductor layer. In another embodiment, the gate electrode of the second field effect transistor is formed concurrently with the gate electrode of the first field effect transistor by deposition and patterning of a gate electrode layer. The first field effect transistor may be a high performance device and the second field effect transistor may be a high voltage device. A design structure for the semiconductor structure is also provided.

    摘要翻译: 第一场效应晶体管包括栅极电介质和位于绝缘体上半导体(SOI))衬底中顶部半导体层的第一部分上方的栅电极。 第二场效应晶体管包括掩埋绝缘体层的一部分和位于掩埋绝缘体层下方的源区和漏区。 在一个实施例中,第二场效应晶体管的栅电极是顶部半导体层的剩余部分。 在另一个实施例中,第二场效应晶体管的栅极通过栅极电极层的沉积和图案化与第一场效应晶体管的栅电极同时形成。 第一场效应晶体管可以是高性能器件,第二场效应晶体管可以是高电压器件。 还提供了用于半导体结构的设计结构。

    Design structure with a deep sub-collector, a reach-through structure and trench isolation
    68.
    发明授权
    Design structure with a deep sub-collector, a reach-through structure and trench isolation 有权
    具有深子集电极的设计结构,通孔结构和沟槽隔离

    公开(公告)号:US08015538B2

    公开(公告)日:2011-09-06

    申请号:US11941104

    申请日:2007-11-16

    CPC分类号: H01L29/0821 H01L29/66272

    摘要: The invention relates to noise isolation in semiconductor devices, and a design structure on which a subject circuit resides. A design structure is embodied in a machine readable medium used in a design process. The design structure includes a deep sub-collector located in a first epitaxial layer, and a doped region located in a second epitaxial layer, which is above the first epitaxial layer. The design structure further includes a reach-through structure penetrating from a surface of the device through the first and second epitaxial layers to the deep sub-collector, and a trench isolation structure penetrating from a surface of the device and surrounding the doped region.

    摘要翻译: 本发明涉及半导体器件中的噪声隔离以及被摄体电路所在的设计结构。 设计结构体现在在设计过程中使用的机器可读介质中。 该设计结构包括位于第一外延层中的深子集电极和位于第一外延层之上的第二外延层中的掺杂区域。 该设计结构进一步包括从装置的表面穿过第一外延层和第二外延层到达深亚集电体的通孔结构,以及从该器件的表面穿透且围绕掺杂区域的沟槽隔离结构。

    METHOD OF FORMING A HIGH PERFORMANCE FET AND A HIGH VOLTAGE FET ON A SOI SUBSTRATE
    70.
    发明申请
    METHOD OF FORMING A HIGH PERFORMANCE FET AND A HIGH VOLTAGE FET ON A SOI SUBSTRATE 有权
    在SOI衬底上形成高性能FET和高电压FET的方法

    公开(公告)号:US20100035390A1

    公开(公告)日:2010-02-11

    申请号:US12188366

    申请日:2008-08-08

    IPC分类号: H01L21/84

    摘要: A first portion of a top semiconductor layer of a semiconductor-on-insulator (SOI) substrate is protected, while a second portion of the top semiconductor layer is removed to expose a buried insulator layer. A first field effect transistor including a gate dielectric and a gate electrode located over the first portion of the top semiconductor layer is formed. A portion of the exposed buried insulator layer is employed as a gate dielectric for a second field effect transistor. In one embodiment, the gate electrode of the second field effect transistor is a remaining portion of the top semiconductor layer. In another embodiment, the gate electrode of the second field effect transistor is formed concurrently with the gate electrode of the first field effect transistor by deposition and patterning of a gate electrode layer.

    摘要翻译: 保护绝缘体上半导体(SOI)衬底的顶部半导体层的第一部分,同时去除顶部半导体层的第二部分以暴露掩埋的绝缘体层。 形成包括位于顶部半导体层的第一部分上方的栅极电介质和栅电极的第一场效应晶体管。 暴露的掩埋绝缘体层的一部分用作第二场效应晶体管的栅极电介质。 在一个实施例中,第二场效应晶体管的栅电极是顶部半导体层的剩余部分。 在另一个实施例中,第二场效应晶体管的栅极通过栅极电极层的沉积和图案化与第一场效应晶体管的栅电极同时形成。