中国物理B ›› 2010, Vol. 19 ›› Issue (6): 66103-066103.doi: 10.1088/1674-1056/19/6/066103

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Degradation mechanisms of current gain in NPN transistors

兰慕杰1, 李兴冀2, 耿洪滨2, 杨德庄2, 何世禹2, 刘超铭2   

  1. (1)School of Astronautics, Harbin Institute of Technology, Harbin 150001, China; (2)Space Materials and Environment Engineering Laboratory, Harbin Institute of Technology, Harbin 150001, China
  • 收稿日期:2009-09-17 出版日期:2010-06-15 发布日期:2010-06-15
  • 基金资助:
    Project supported by the National Basic Research Program of China (Grant No.~61343).

Degradation mechanisms of current gain in NPN transistors

Li Xing-Ji(李兴冀)a)†, Geng Hong-Bin(耿洪滨)a), Lan Mu-Jie(兰慕杰)b), Yang De-Zhuang(杨德庄)a), He Shi-Yu(何世禹) a), and Liu Chao-Ming(刘超铭)a)   

  1. a Space Materials and Environment Engineering Laboratory, Harbin Institute of Technology, Harbin 150001, China; b School of Astronautics, Harbin Institute of Technology, Harbin 150001, China
  • Received:2009-09-17 Online:2010-06-15 Published:2010-06-15
  • Supported by:
    Project supported by the National Basic Research Program of China (Grant No.~61343).

摘要: An investigation of ionization and displacement damage in silicon NPN bipolar junction transistors (BJTs) is presented. The transistors were irradiated separately with 90-keV electrons, 3-MeV protons and 40-MeV Br ions. Key parameters were measured {\em in-situ} and the change in current gain of the NPN BJTS was obtained at a fixed collector current (I_{\rm c}=1~mA). To characterise the radiation damage of NPN BJTs, the ionizing dose D_{\i} and displacement dose D_{\d} as functions of chip depth in the NPN BJTs were calculated using the SRIM and Geant4 code for protons, electrons and Br ions, respectively. Based on the discussion of the radiation damage equation for current gain, it is clear that the current gain degradation of the NPN BJTs is sensitive to both ionization and displacement damage. The degradation mechanism of the current gain is related to the ratio of D_{\rm d}/(D_{\rm d}+D_{\rm i}) in the sensitive region given by charged particles. The irradiation particles leading to lower D_{\rm d}/(D_{\rm d}+D_{\rm i}) within the same chip depth at a given total dose would mainly produce ionization damage to the NPN BJTs. On the other hand, the charged particles causing larger D_{\rm d}/(D_{\rm d}+D_{\rm i}) at a given total dose would tend to generate displacement damage to the NPN BJTs. The Messenger--Spratt equation could be used to describe the experimental data for the latter case.

Abstract: An investigation of ionization and displacement damage in silicon NPN bipolar junction transistors (BJTs) is presented. The transistors were irradiated separately with 90-keV electrons, 3-MeV protons and 40-MeV Br ions. Key parameters were measured in-situ and the change in current gain of the NPN BJTS was obtained at a fixed collector current ($I_{\rm c}=1$ mA). To characterise the radiation damage of NPN BJTs, the ionizing dose $D_{\rm i}$ and displacement dose $D_{\rm d}$ as functions of chip depth in the NPN BJTs were calculated using the SRIM and Geant4 code for protons, electrons and Br ions, respectively. Based on the discussion of the radiation damage equation for current gain, it is clear that the current gain degradation of the NPN BJTs is sensitive to both ionization and displacement damage. The degradation mechanism of the current gain is related to the ratio of $D_{\rm d}/(D_{\rm d}+D_{\rm i}$) in the sensitive region given by charged particles. The irradiation particles leading to lower $D_{\rm d}/(D_{\rm d}+D_{\rm i}$) within the same chip depth at a given total dose would mainly produce ionization damage to the NPN BJTs. On the other hand, the charged particles causing larger $D_{\rm d}/(D_{\rm d}+D_{\rm i})$ at a given total dose would tend to generate displacement damage to the NPN BJTs. The Messenger--Spratt equation could be used to describe the experimental data for the latter case.

Key words: radiation effects, ionization damage, displacement damage, transistors

中图分类号:  (Bipolar transistors)

  • 85.30.Pq
85.30.De (Semiconductor-device characterization, design, and modeling) 61.80.Fe (Electron and positron radiation effects) 61.80.Jh (Ion radiation effects)