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    • 6. 发明授权
    • Circuit simulation of MOSFETs
    • MOSFET的电路仿真
    • US08731893B2
    • 2014-05-20
    • US13080154
    • 2011-04-05
    • Mitiko Miura-MattauschNorio SadachikaShunta KusuTakaki Yoshida
    • Mitiko Miura-MattauschNorio SadachikaShunta KusuTakaki Yoshida
    • G06F17/50
    • G06F17/5036
    • An arithmetic device calculates the surface potential of a silicon layer by performing computation based on a mathematical expression and device parameters stored in a storage device. Likewise, the arithmetic device calculates the surface potential of a bulk layer under a buried oxide film when the silicon layer is in a partially depleted state and when the silicon is in a fully depleted state. The arithmetic device then performs computation based on the calculated surface potential of the silicon layer, the calculated surface potential of the bulk layer, and mathematical expressions stored in the storage device, and obtains the surface potential of the bulk layer by iterative calculation. The arithmetic device performs computation based on the surface potential of the bulk layer obtained by iterative calculation and mathematical expressions stored in the storage device, and calculates the lower surface potential of the silicon layer.
    • 算术装置通过基于存储在存储装置中的数学表达式和装置参数进行计算来计算硅层的表面电位。 同样,当硅层处于部分耗尽状态时,当硅处于完全耗尽状态时,算术装置计算掩埋氧化膜下的体层的表面电位。 然后,运算装置根据计算出的硅层的表面电位,体积层的计算出的表面电位,存储在存储装置中的数学式进行计算,通过迭代计算得到体层的表面电位。 算术装置根据通过迭代计算获得的体层的表面电位和存储在存储装置中的数学表达式进行计算,并计算硅层的下表面电位。
    • 9. 发明申请
    • SIMULATION METHOD AND SIMULATION APPARATUS
    • 模拟方法和仿真设备
    • US20110184708A1
    • 2011-07-28
    • US13080154
    • 2011-04-05
    • Mitiko MIURA-MATTAUSCHNorio SadachikaShunta KusuTakaki Yoshida
    • Mitiko MIURA-MATTAUSCHNorio SadachikaShunta KusuTakaki Yoshida
    • G06F17/50G06F7/60
    • G06F17/5036
    • An arithmetic device calculates the surface potential of a silicon layer by performing computation based on a mathematical expression and device parameters stored in a storage device. Likewise, the arithmetic device calculates the surface potential of a bulk layer under a buried oxide film when the silicon layer is in a partially depleted state and when the silicon is in a fully depleted state. The arithmetic device then performs computation based on the calculated surface potential of the silicon layer, the calculated surface potential of the bulk layer, and mathematical expressions stored in the storage device, and obtains the surface potential of the bulk layer by, iterative calculation. The arithmetic device performs computation based on the surface potential of the bulk layer obtained by iterative calculation and mathematical expressions stored in the storage device, and calculates the lower surface potential of the silicon layer.
    • 算术装置通过基于存储在存储装置中的数学表达式和装置参数进行计算来计算硅层的表面电位。 同样,当硅层处于部分耗尽状态时,当硅处于完全耗尽状态时,算术装置计算掩埋氧化膜下的体层的表面电位。 运算装置然后根据计算出的硅层表面电位,体积层的计算出的表面电位和存储在存储装置中的数学式进行计算,并通过迭代计算得到体层的表面电位。 算术装置根据通过迭代计算获得的体层的表面电位和存储在存储装置中的数学表达式进行计算,并计算硅层的下表面电位。
    • 10. 发明授权
    • Simulation model for a semiconductor device describing a quasi-static density of a carrier as a non-quasi-static model
    • 用于描述作为非准静态模型的载波的准静态密度的半导体器件的仿真模型
    • US07343571B2
    • 2008-03-11
    • US10933335
    • 2004-09-03
    • Mitiko MiuraNoriaki Nakayama
    • Mitiko MiuraNoriaki Nakayama
    • G06F17/59H03K17/693G01R31/26
    • G06F17/5036
    • There is disclosed a simulation model for designing a semiconductor device, comprising adding at least a part of a difference between a density of a carrier described in a quasi-static manner with respect to a voltage applied between electrodes at a first time and a density of the carrier described in a transient state at a second time before the first time to the carrier density at the second time in accordance with a running delay of the carrier between both the times to thereby describe the carrier density at the first time in the transient state with respect to a semiconductor element having the first and second electrodes. A current flowing between the electrodes is described as a sum of a current flowing between the electrodes in the quasi-static manner, and a displacement current between the electrodes.
    • 公开了一种用于设计半导体器件的仿真模型,包括:以准静态方式描述的载流子的密度相对于在第一时间施加在电极之间的电压和至少一个 载波在第一时间之前的第二时间根据两个时间之间的载波的运行延迟在第二时间处于暂态状态下描述为载波密度,从而描述在瞬时状态下的第一时间的载波密度 相对于具有第一和第二电极的半导体元件。 在电极之间流动的电流被描述为以静态方式在电极之间流动的电流和电极之间的位移电流之和。