H+ implantation profile formation in m:Cz and Fz silicon

S. Kirnstoetter, M. Faccinelli, P. Hadley, M. Jelinek, W. Schustereder, J. Laven, H. Schulze
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引用次数: 2

Abstract

Implanting hydrogen ions (H+) into silicon creates defects that can act as donors. The microscopic structure of these defects is not entirely clear. There is a difference in the resulting doping profiles if the silicon is produced by the float zone (Fz) process or the magnetic Czochralski (m:Cz) process. Silicon produced by the m:Cz process has higher concentrations of oxygen and carbon than silicon produced by the Fz process. The presence of the oxygen and carbon affects the formation of defects and thereby the doping profile. We implanted high resistivity p-type m:Cz and Fz wafers with protons. Due to the n-type doping from the H+ implantation, a pn-junction was generated in the sample. Simulations indicate that the H+ implantation depth is 148 μm. Spreading Resistance Profiling (SRP) measurements of as-implanted and not annealed samples show a donor peak at 148 μm in the Fz samples but the peak is at about 160 μm depth in m:Cz samples. After a low temperature anneal of the m:Cz samples at temperatures between 150 and 250 °C for at least 30 minutes, the expected end of range (EOR) donor peak (at about 148 μm) appears. For higher annealing temperatures, the hydrogen related donor complexes (HTD's) become activated and the EOR peak becomes dominant in the implantation profile. In an SRP study we show the evolution of the doping profile of hydrogen implanted m:Cz and Fz wafers as a function of the annealing temperature. To monitor the depth of the formed pn-junction and the effective local diffusion length in the proton radiation damaged region, Electron Beam Induced Current (EBIC) measurements were performed.
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m:Cz和Fz硅中H+注入分布的形成
将氢离子(H+)植入硅中会产生缺陷,充当供体。这些缺陷的显微结构还不完全清楚。如果硅是由浮子区(Fz)工艺或磁性Czochralski (m:Cz)工艺生产的,则所得到的掺杂曲线是不同的。用m:Cz工艺生产的硅比用Fz工艺生产的硅含有更高浓度的氧和碳。氧和碳的存在影响缺陷的形成,从而影响掺杂谱。我们用质子注入高电阻率p型m:Cz和Fz晶圆。由于H+注入的n型掺杂,在样品中产生了一个pn结。模拟结果表明,H+注入深度为148 μm。对注入和未退火样品的扩展电阻谱(SRP)测量表明,Fz样品的供体峰位于148 μm处,而m:Cz样品的供体峰位于约160 μm处。将m:Cz样品在150 ~ 250℃的温度下低温退火至少30分钟后,出现了预期的EOR供体峰(约148 μm)。在较高的退火温度下,氢相关的供体配合物(HTD)被激活,EOR峰在注入剖面中占据主导地位。在SRP研究中,我们展示了氢注入m:Cz和Fz晶圆的掺杂谱随退火温度的变化。为了监测形成的pn结的深度和质子辐射损伤区的有效局部扩散长度,进行了电子束感应电流(EBIC)测量。
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