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硅光电二极管响应率SPICE模型
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作者 吉红 《中国高新技术企业》 2007年第13期76-76,81,共2页
本文给出了一种硅光电二极管响应率模型,考虑由于前区的非均匀掺杂引起的少子非均匀分布,分析了响应率相对于该少子分布的积分表达,在高斯分布近似下,在SPICE中完成了整个硅光电二级管的响应率模型,分析其分布参数对响应率影响,而后通... 本文给出了一种硅光电二极管响应率模型,考虑由于前区的非均匀掺杂引起的少子非均匀分布,分析了响应率相对于该少子分布的积分表达,在高斯分布近似下,在SPICE中完成了整个硅光电二级管的响应率模型,分析其分布参数对响应率影响,而后通过与实验数据比较,验证模型的有效性。 展开更多
关键词 硅光二极管 响应率 SPICE模型 前区 少子分布
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Carrier dynamics and doping profiles in GaAs nanosheets 被引量:1
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作者 Chia-Chi Chang Chun-Yung Chi +6 位作者 Chun-Chung Chen Ningfeng Huang Shermin Arab Jing Qiu Michelle L. Povinelli P. Daniel Dapkus Stephen B. Cronin 《Nano Research》 SCIE EI CAS CSCD 2014年第2期163-170,共8页
We have recently demonstrated that GaAs nanosheets can be grown by metal-organic chemical vapor deposition (MOCVD). Here, we investigate these nanosheets by secondary electron scanning electron microscopy (SE-SEM)... We have recently demonstrated that GaAs nanosheets can be grown by metal-organic chemical vapor deposition (MOCVD). Here, we investigate these nanosheets by secondary electron scanning electron microscopy (SE-SEM) and electron beam induced current (EBIC) imaging. An abrupt boundary is observed between an initial growth region and an overgrowth region in the nanosheets. The SE-SEM contrast between these two regions is attributed to the inversion of doping at the boundary. EBIC mapping reveals a p-n junction formed along the boundary between these two regions. Rectifying I-V behavior is observed across the boundary further indicating the formation of a p-n junction. The electron concentration (ND) of the initial growth region is around 1 × 10^18 cm^-3, as determined by both Hall effect measurements and low temperature photoluminescence (PL) spectroscopy. Based on the EBIC data, the minority carrier diffusion length of the nanosheets is 177 nm, which is substantially longer than the corresponding length in unpassivated GaAs nanowires measured previously. 展开更多
关键词 MOCVD GAAS NANOSHEETS EBIC Hall measurement secondary electronemission
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