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    • 3. 发明授权
    • Transient gate tunneling current control
    • 瞬态栅极隧道电流控制
    • US06577178B1
    • 2003-06-10
    • US10064504
    • 2002-07-23
    • Kerry BernsteinPeter E. CottrellEdward J. NowakNorman J. RohrerDouglas W. Stout
    • Kerry BernsteinPeter E. CottrellEdward J. NowakNorman J. RohrerDouglas W. Stout
    • H03K1730
    • H03K19/00361H03K19/0948
    • A circuit includes a resistance-capacitance (RC) structure connected to a first set of transistors and a second set of transistors that perform the same logical function as the first set of transistors. The first set of transistors have thinner gate oxides than the second set of transistors. The RC structure drains an electric field from the first set of transistors, such that the first set of transistors are on only during initial transistor switching. In other words, the RC structure turns off the first set of transistors after transistor switching is completed. Also, the first set of transistors and the second set of transistors share common inputs and outputs. The first set of transistors exhibit higher tunneling currents than the second set of transistors. The thinner gate oxides of the first set of transistors cause the first set of transistors to exhibit higher device currents than the second set of transistors. The RC structure includes a capacitor connected to a gate of the first set of transistors and a resistor connected to the capacitor and to ground.
    • 电路包括连接到第一组晶体管的电阻 - 电容(RC)结构和执行与第一组晶体管相同的逻辑功能的第二组晶体管。 第一组晶体管具有比第二组晶体管更薄的栅极氧化物。 RC结构从第一组晶体管引出电场,使得第一组晶体管仅在初始晶体管切换期间导通。 换句话说,在晶体管切换完成之后,RC结构关闭第一组晶体管。 此外,第一组晶体管和第二组晶体管共享公共输入和输出。 第一组晶体管表现出比第二组晶体管更高的隧穿电流。 第一组晶体管的较薄的栅极氧化物导致第一组晶体管表现出比第二组晶体管更高的器件电流。 RC结构包括连接到第一组晶体管的栅极的电容器和连接到电容器并接地的电阻器。
    • 9. 发明授权
    • Channel hot electron monitor
    • 通道热电子监视器
    • US4382229A
    • 1983-05-03
    • US210937
    • 1980-11-28
    • Peter E. CottrellRonald R. Troutman
    • Peter E. CottrellRonald R. Troutman
    • G01R31/26G01R31/22
    • G01R31/2621
    • This teaches that by measuring the rate of change in gate current of an insulating gate field effect transistor, under normal operating conditions, the time required to achieve a predetermined change in source-to-drain current in the transistor can be found. Because changes in gate current depends more on sensitivity on charge trapping in the oxide than do changes in channel current, and since the gate current occurs only in the small region of electron emission, the effects on gate current are more quickly developed than the secondary effect of reduced channel current due to the charge in gate oxide caused by the presence of trapped electrons.
    • 这表明,通过测量绝缘栅场效应晶体管的栅极电流的变化率,在正常工作条件下,可以找到实现晶体管中源极 - 漏极电流的预定变化所需的时间。 因为栅极电流的变化更多地取决于在沟道电流中改变氧化物中的电荷捕获的灵敏度,并且由于栅极电流仅发生在电子发射的小区域中,所以对栅极电流的影响比次级效应更快地发展 由于俘获电子的存在引起的栅极氧化物中的电荷引起的沟道电流减小。
    • 10. 发明授权
    • Simple process for making complementary transistors
    • 制造互补晶体管的简单过程
    • US4480375A
    • 1984-11-06
    • US448124
    • 1982-12-09
    • Peter E. CottrellHenry J. Geipel, Jr.
    • Peter E. CottrellHenry J. Geipel, Jr.
    • H01L27/092H01L21/8238H01L29/78H01L21/22H01L21/263
    • H01L21/823814Y10S438/981
    • A very simple process is provided, with reduced processing time, for making a CMOS structure using a single polysilicon, or other refractory metal, layer which includes forming a thin gate oxide on both N and P type semiconductor layers of a common substrate, forming a gate electrode simultaneously on the N type and on the P type layers and selectively implanting an N type impurity to form N+ source and drain regions in the P type layer. The semiconductor layers are then oxidized to form substantially thicker oxide, such a silicon dioxide, adjacent to the sides of the gate electrode over the P type layer than the thickness of the oxide adjacent to the sides of the gate electrode over the N type layer. Without using a mask, a P type impurity is implanted into the N type layer to form P+ source and drain regions.
    • 提供了一种非常简单的方法,缩短了处理时间,用于制造使用单个多晶硅的CMOS结构或其它难熔金属层,其包括在公共基板的N型和P型半导体层上形成薄的栅极氧化物,形成 栅电极同时在N型和P型层上,并且选择性地注入N型杂质以在P型层中形成N +源极和漏极区。 然后氧化氧化半导体层以形成比在N型层上与栅电极相邻的氧化物的厚度相邻的,比P型层更靠近栅电极侧面的基本上较厚的氧化物,例如二氧化硅。 在不使用掩模的情况下,将P型杂质注入到N型层中以形成P +源极和漏极区。