会员体验
专利管家(专利管理)
工作空间(专利管理)
风险监控(情报监控)
数据分析(专利分析)
侵权分析(诉讼无效)
联系我们
交流群
官方交流:
QQ群: 891211   
微信请扫码    >>>
现在联系顾问~
热词
    • 2. 发明申请
    • BIPOLAR-TRANSISTOR AND METHOD FOR THE PRODUCTION OF A BIPOLAR-TRANSISTOR
    • 双极型晶体管及其制造方法双极晶体管
    • WO2005098960A3
    • 2006-04-20
    • PCT/EP2005003129
    • 2005-03-24
    • PREMA SEMICONDUCTOR GMBHGRUETZEDIEK HARTMUTRAMMENSEE MICHAELSCHEERER JOACHIM
    • GRUETZEDIEK HARTMUTRAMMENSEE MICHAELSCHEERER JOACHIM
    • H01L29/732H01L21/331H01L29/06H01L29/08
    • H01L29/66272H01L29/0615H01L29/0821H01L29/7322
    • The invention relates to NPN and PNP bipolar transistors and to a method for the production thereof, said transistors being characterised by a particularly high collector-emitter and collector-base blocking voltage. The blocking voltage is increased by a particular doping profile. An NPN bipolar transistor comprises a p-doped substrate (1), a trenched n-doped layer (3) forming the collector, a p-doped layer (7) which is arranged above the trenched n-doped layer and is made of a base and an n-doped layer which is arranged within the p-doped layer and forms an emitter of the transistor. A spatial charge area (RLZ 1) is formed between the p-doped layer and the trenched n-doped layer and a second spatial charge area (RLZ 2) is formed between the trenched n-doped layer and the p-doped substrate, which expands in the vertical direction on the collector when the transistor is operated with an increasing potential. The trenched n-doped layer comprises a doping profile in such a manner that when the transistor is operated with an increasing potential, the first and the second spatial charge area expand on the collector, transversing the entire depth of the trenched n-doped layer prior to the critical field strength for a breakthrough being reached between the collector and emitter.
    • 本发明涉及一种NPN和PNP双极型晶体管及其制造相同,其特征在于特别高的集电极 - 发射极和集电极 - 基极反向电压的方法。 在反向电压的增加是通过特殊掺杂分布来实现的。 在具有p型掺杂的衬底1,掩埋的n型层3所形成的集电极,一个掩埋n型层布置p掺杂层参照图7,基座上方并设置在p掺杂层的n掺杂层内的NPN型双极晶体管 所述晶体管的发射极。 形成有p型掺杂层和掩埋的n型层和第二空间电荷区RLZ 2之间的第一空间电荷区RLZ 1之间的掩埋的n型层和p型衬底从与增大的电势的晶体管的操作期间 延伸在一个垂直方向上的集电体。 掩埋n型层具有掺杂分布,其被创建,使得与在集电极增加潜在扩大第一和第二空间电荷区,掩埋n型层为临界场强之前整个深度的晶体管的操作期间的渗透 到达集电极和发射极之间的击穿。