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    • 5. 发明申请
    • BURIED SUBCOLLECTOR FOR HIGH FREQUENCY PASSIVE DEVICES
    • 用于高频无源器件的BURIED SUBCOLLECTOR
    • US20070105354A1
    • 2007-05-10
    • US11164108
    • 2005-11-10
    • Douglas CoolbaughXuefeng LiuRobert RasselDavid Sheridan
    • Douglas CoolbaughXuefeng LiuRobert RasselDavid Sheridan
    • H01L21/425
    • H01L21/8249H01L29/0821H01L29/66272
    • A method of fabricating a buried subcollector in which the buried subcollector is implanted to a depth in which during subsequent epi growth the buried subcollector remains substantially below the fictitious interface between the epi layer and the substrate is provided. In particular, the inventive method forms a buried subcollector having an upper surface (i.e., junction) that is located at a depth from about 3000 Å or greater from the upper surface of the semiconductor substrate. This deep buried subcollector having an upper surface that is located at a depth from about 3000 Å or greater from the upper surface of the substrate is formed using a reduced implant energy (as compared to a standard deep implanted subcollector process) at a relative high dose. The present invention also provides a semiconductor structure including the inventive buried subcollector which can be used as cathode for passive devices in high frequency applications.
    • 一种制造掩埋子集电极的方法,其中将埋入的子集电极注入深度,其中在随后的外延生长期间,掩埋子集电极基本上保持在外延层和衬底之间的虚拟界面的下方。 特别地,本发明的方法形成了具有从半导体衬底的上表面位于距离大约或更大的深度的上表面(即结)的掩埋子集电极。 该深埋底部集电器具有从衬底的上表面位于距离大约等于或更大的深度的上表面,其使用相对高剂量的减少的注入能量(与标准深度植入子集电极过程相比) 。 本发明还提供了一种半导体结构,其包括本发明的掩埋子集电极,其可以用作高频应用中的无源器件的阴极。
    • 9. 发明申请
    • MOS VARACTOR USING ISOLATION WELL
    • 使用隔离的MOS变压器
    • US20060043454A1
    • 2006-03-02
    • US10711144
    • 2004-08-27
    • Douglas CoolbaughDouglas HershbergerRobert Rassel
    • Douglas CoolbaughDouglas HershbergerRobert Rassel
    • H01L29/94H01L21/20
    • H01L29/93H01L29/94
    • The present invention provides a varactor that has increased tunability and a high quality factor Q as well as a method of fabricating the varactor. The method of the present invention can be integrated into a conventional CMOS processing scheme or into a conventional BiCMOS processing scheme. The method includes providing a structure that includes a semiconductor substrate of a first conductivity type and optionally a subcollector or isolation well (i.e., doped region) of a second conductivity type located below an upper region of the substrate, the first conductivity type is different from said second conductivity type. Next, a plurality of isolation regions are formed in the upper region of the substrate and then a well region is formed in the upper region of the substrate. In some cases, the doped region is formed at this point of the inventive process. The well region includes outer well regions of the second conductivity type and an inner well region of the first conductivity type. Each well of said well region is separated at an upper surface by an isolation region. A field effect transistor having at least a gate conductor of the first conductivity type is then formed above the inner well region.
    • 本发明提供一种具有增加的可调性和高品质因数Q的变容二极管以及制造变容二极管的方法。 本发明的方法可以集成到常规的CMOS处理方案中,或者被整合到常规的BiCMOS处理方案中。 该方法包括提供包括第一导电类型的半导体衬底和位于衬底的上部区域下方的第二导电类型的子集电极或隔离阱(即,掺杂区)的结构,第一导电类型不同于 所述第二导电类型。 接下来,在基板的上部区域形成多个隔离区域,然后在基板的上部区域形成阱区域。 在一些情况下,在本发明方法的这一点形成掺杂区域。 阱区包括第二导电类型的外阱区和第一导电类型的内阱区。 所述阱区的每个阱在上表面被隔离区分开。 然后形成至少具有第一导电类型的栅极导体的场效应晶体管,并在内部阱区域的上方形成。
    • 10. 发明申请
    • RESISTOR TUNING
    • 电阻调谐
    • US20050230785A1
    • 2005-10-20
    • US10709115
    • 2004-04-14
    • Douglas CoolbaughEbenezer EshunRobert RasselAnthony Stamper
    • Douglas CoolbaughEbenezer EshunRobert RasselAnthony Stamper
    • H01C17/26H01L29/76
    • H01C17/267
    • A structure for resistors and the method for tuning the same. The resistor comprises an electrically conducting region coupled to a liner region. Both the electrically conducting region and the liner region are electrically coupled to first and second contact regions. A voltage difference is applied between the first and second contact regions. As a result, a current flows between the first and second contact regions in the electrically conducting region. The voltage difference and the materials of the electrically conducting region and the liner region are such that electromigration occurs only in the electrically conducting region. As a result, a void region within the electrically conducting region expands in the direction of the flow of the charged particles constituting the current. Because the resistor loses a conducting portion of the electrically conducting region to the void region, the resistance of the resistor is increased (i.e., tuned).
    • 电阻器结构及其调谐方法。 电阻器包括耦合到衬垫区域的导电区域。 导电区域和衬里区域都电耦合到第一和第二接触区域。 在第一和第二接触区域之间施加电压差。 结果,电流在导电区域中的第一和第二接触区域之间流动。 导电区域和衬垫区域的电压差和材料使得电迁移仅在导电区域中发生。 结果,导电区域内的空隙区域在构成电流的带电粒子的流动方向上膨胀。 因为电阻器将导电区域的导电部分损失到空隙区域,电阻器的电阻增加(即调谐)。