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首页> 外文期刊>Physical Review, B. Condensed Matter >DIVACANCY AND RESISTIVITY PROFILES IN N-TYPE SI IMPLANTED WITH 1.15-MEV PROTONS
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DIVACANCY AND RESISTIVITY PROFILES IN N-TYPE SI IMPLANTED WITH 1.15-MEV PROTONS

机译:植入1.15-MEV质子的N型SI的导磁率和电阻率曲线

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摘要

Defect profiles were determined in proton-implanted low-doped ([P]=1X10(14) cm(-3)) n-type silicon layers by performing positron-electron pair momentum-distribution measurements with a slow-positran beam, conventional positron lifetime, and e(+)-e(-) pair momentum-distribution measurements with a Na-22-source and spreading resistance measurements. The dominant positron trap induced by 1.15 and 3.0 MeV proton implantations is the silicon divacancy V-2. Compared to the values in bulk, the characteristic positron lifetime and the characteristic low- and high-momentum parameters of the e(+)-e(-) pair momentum distribution at the divacancy are tau(d)=300 ps=1.35 tau(b), S-d=1.052S(b), and W-d=0.78W(b), respectively. The divacancy is observed in the negative charge state V-2(-). The divacaney profile is determined in n-type Si implanted with 1.15-MeV (20 mu m) protons to a dose 1X10(14) cm(-2) and the maximum concentration [V-2(-)]=4-8X10(15) cm(-3) is observed at depths 16-18 mu m. The resistivity increases with increasing divacancy concentration. After annealing at 400 degrees C the spreading resistance measurements reveal a region of shallow hydrogen-related donors at depths 15-21 mu m. The positron annihilation results support the idea that the introduction of shallow donors is due to the formation of hydrogen-vacancy complexes during the annealing. [References: 40]
机译:通过使用慢正电子束,常规正电子执行正电子-电子对动量分布测量,确定质子注入的低掺杂([P] = 1X10(14)cm(-3))n型硅层中的缺陷分布寿命,以及e(+)-e(-)对动量分布测量与Na-22源和扩散阻力测量。由1.15和3.0 MeV质子注入引起的主要正电子陷阱是硅空位V-2。与散装值相比,在空位处e(+)-e(-)对动量分布的特征正电子寿命和特征动量低和高动量参数为tau(d)= 300 ps = 1.35 tau( b),Sd = 1.052S(b)和Wd = 0.78W(b)。在负电荷状态V-2(-)中观察到了空位。 divacaney轮廓是在n型Si中植入1.15-MeV(20μm)质子至剂量1X10(14)cm(-2)且最大浓度[V-2(-)] = 4-8X10( 15)cm(-3)在16-18微米的深度处观察到。电阻率随着空位浓度的增加而增加。在400摄氏度下退火后,扩展电阻测量显示深度为15-21微米的浅氢相关供体区域。正电子an没的结果支持以下观点:引入浅施主是由于退火期间氢空位络合物的形成。 [参考:40]

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