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    • 4. 发明授权
    • Ion current density measuring method and instrument, and semiconductor device manufacturing method
    • 离子电流密度测量方法和仪器,以及半导体器件制造方法
    • US06656752B1
    • 2003-12-02
    • US09890611
    • 2001-10-11
    • Nobuyuki MiseTatehito UsuiMasato IkegawaKazuo NojiriKazuyuki TsunokuniTetsuo Ono
    • Nobuyuki MiseTatehito UsuiMasato IkegawaKazuo NojiriKazuyuki TsunokuniTetsuo Ono
    • H01L2166
    • H01L22/34
    • A wafer is exposed to a plasma. Here, the wafer includes a semiconductor or a conductor 1 provided on an insulator 6, an insulator 2 formed thereon and having a region the thickness of which has been made locally thin, and a 2nd conductor 4 provided on the insulator 2, one of the semiconductor or the conductor 1 and the 2nd conductor 4 having a 1st region from the surface of which a substantially total solid angle is formed, the other having a 2nd region a solid angle formed from the surface of which is made smaller than the 1st region. Then, a voltage is applied to the semiconductor or the conductor 1 and the 2nd conductor 4 so as to measure a time elapsing until the insulator 2 undergoes a dielectric breakdown. Moreover, the ion current density is determined from an electric charge required therefor and an area exposed onto the surface of the 2nd conductor 4. Consequently, it becomes possible to measure, on the wafer, the current density of the ions launched into the wafer, thereby allowing the measuring method of the icon current density to be made suitable for the mass production.
    • 将晶片暴露于等离子体。 这里,晶片包括设置在绝缘体6上的半导体或导体1,形成在其上的绝缘体2,其厚度局部变薄的区域和设置在绝缘体2上的第二导体4, 半导体或导体1和第二导体4具有从其表面基本上具有总立体角的第一区域,另一个具有从其表面形成的立体角小于第一区域的第二区域。 然后,向半导体或导体1和第二导体4施加电压,以测量直到绝缘体2经历介电击穿的时间。 此外,离子电流密度由其所需的电荷和暴露于第二导体4的表面的面积确定。因此,可以在晶片上测量发射到晶片中的离子的电流密度, 从而允许图标电流密度的测量方法适合于批量生产。