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传统 PECVD高品质氢化非晶硅的淀积率 被引量:1

The Deposition Rate of the High-quality Hydrogenated Amorphous Silicon Prepared by the Conventional PECVD Process
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摘要 根据 Winer模型 ,联合 Winer模型和 Street的氢化学势理论 ,分别研究了传统 PECVD( CPECVD)高品质氢化非晶硅 ( HQ a-Si:H)的淀积率上限 rdup和淀积率 rd 与 a-Si:H缺陷密度 ND 的关系。得到的结论是 :( 1 )rdup=1 .6nm/s(目前实验上 rd 已接近 1 .0 nm/s)。( 2 )对每一优化淀积温度 ( Ts=2 0 0~ 30 0°C) ,存在一相应的优化淀积率 rdop,当 rd<rdop时 ,rd 增加 ,ND减小 (解释了 Tsuda etal的实验曲线的左边 )。还讨论了在大淀积率下( 0 .5 nm/s<rd<rdup)制备 HQ a-Si:H时避免粉末形成的可能方法。结果显示 :适当功率密度 Pd/Si H4 流速率 fr和 (或 )适当的 Si H4 气压 Pr/fr匹配是至关重要的。 Following Winer model combining Street's hydrogen chemical potential, we have investigated respectively the upper limited of deposition rate, r_(dup), of the high quality a-Si:H prepared by the conventoinal PECVD (CPECVD) as well as the relation between the CPECVD a-Si:H defect density, N_D, and its deposition rate, r_d. The resulting conclusions are:(1)r_(dup)=1.6 nm/s. At present, r_(dup) have approached experimentally to 1.0 nm/s.(2)For each optimal deposition temperature (200~300(°C)), there is a correspondent optimal deposition rate,r_(dop). On the condition of r_d<r_(dop), when r_dincrease, N_Ddecrease. This is just the left property of Tsuda et al's experimental curve (250(°C)).At last, we discuss the polymer reaction and powder formation under the high r_d (>0.5 nm/s). It is shown that, in roder to avoid these disadvantages, the suitable matching of the power density P_d/SiH_4flow rate and/or SiH_4pressure P_r/f_rare the decisive importance factor.
作者 颜一凡
机构地区 湖南大学物理系
出处 《固体电子学研究与进展》 CAS CSCD 北大核心 2004年第3期402-406,共5页 Research & Progress of SSE
关键词 非晶硅 等离子增强化学气相淀积 淀积率上限 优化淀积率 amorphous silicon conventional PECVD upper limite of deposition rate optimal deposition rate
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  • 1Conde J P,J Appl Phys,1992年,71卷,8期,3981页
  • 2Cabarrocas P Rocai,Non Cryst Solids,1989年,114卷,1期,190页
  • 3Lucovsky G,Non-Cryst Solids,1987年,1997/1998卷,1期,265页

同被引文献8

  • 1Kushner M J. A Model for the Discharge Kinetics and Plasma Chemistry during Plasma PECVD of Amorphous Silicon[J]. J Appl Phys, 1988, 63(8):2532-2551.
  • 2Shin-inchiro Ishihara. Effects of Discharge Parameters on Deposition Rate of Hydrogenated Amorphous Silicon for Solar Cells from Pure SiH4 Plasma[J]. J Appl Phys, 1987,62(2) : 485-491.
  • 3李国光 杨恒青 黄家明 等.用透射光谱确定非晶硅薄膜的厚度和光学参数.红外研究,1987,6(5):321-328.
  • 4Kampas F J. Reactions of Hydrogen in the Deposition of Hydrogenated Amorphous Silicon by Glow Discharge and Reactive Sputtering[J]. J Appl Phys, 1982,53(9):6408-6412.
  • 5Matsuda A. Amorphous Si and Si-based Alloys from Glow-discharge[J]. Plasma Pure& Appl Chem, 1988,60 (5) :733-740.
  • 6Itzhak Webman, Joshua Jortner, Morrel H Cohen. Theory of Optical and Microwave Properties of Microscopically Inhomogehey)us Materials[J]. Phys Rev B, 1977,15(12) :5712-5723.
  • 7韩大星,王万录,张智.非晶硅电致发光机理及用电致发光谱研究太阳能电池本征层中的缺陷态能量分布[J].物理学报,1999,48(8):1484-1490. 被引量:7
  • 8余云鹏,林舜辉,黄翀,林璇英.非晶硅薄膜厚度均匀性对其透射光谱的影响[J].汕头大学学报(自然科学版),2004,19(1):50-54. 被引量:6

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