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通过镍电沉积制备用于太阳能电池的无切口剥离薄硅片

Kerf-Less Exfoliated Thin Silicon Wafer Prepared by Nickel Electrodeposition for Solar Cells.

作者信息

Yang Hyun-Seock, Kim Jiwon, Kim Seil, Eom Nu Si A, Kang Sangmuk, Han Chang-Soon, Kim Sung Hae, Lim Donggun, Lee Jung-Ho, Park Sung Heum, Choi Jin Woo, Lee Chang-Lyoul, Yoo Bongyoung, Lim Jae-Hong

机构信息

Electrochemistry Department, Korea Institute of Materials Science, Changwon, South Korea.

Department of Physics, Pukyong National University Busan, South Korea.

出版信息

Front Chem. 2019 Jan 14;6:600. doi: 10.3389/fchem.2018.00600. eCollection 2018.

DOI:10.3389/fchem.2018.00600
PMID:30693277
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC6339913/
Abstract

Ultra-thin and large-area silicon wafers with a thickness in the range of 20-70 μm, were produced by spalling using a nickel stressor layer. A new equation for predicting the thickness of the spalled silicon was derived from the Suo-Hutchinson mechanical model and the kinking mechanism. To confirm the reliability of the new equation, the proportional factor of stress induced by the nickel on the silicon wafer, was calculated. The calculated proportional factor of λ = 0.99 indicates that the thickness of the spalled silicon wafer is proportional to that of the nickel layer. A similar relationship was observed in the experimental data obtained in this study. In addition, the thickness of the stressor layer was converted to a value of stress as a guide when using other deposition conditions and materials. A silicon wafer with a predicted thickness of 50 μm was exfoliated for further analysis. In order to spall a large-area (150 × 150 mm or 6 × 6 in) silicon wafer without kerf loss, initial cracks were formed by a laser pretreatment at a proper depth (50 μm) inside the exfoliated silicon wafer, which reduced the area of edge slope (kerf loss) from 33 to 3 mm. The variations in thickness of the spalled wafer remained under 4%. Moreover, we checked the probability of degradation of the spalled wafers by using them to fabricate solar cells; the efficiency and ideality factor of the spalled silicon wafers were found to be 14.23%and 1.35, respectively.

摘要

通过使用镍应力层剥落法制备了厚度在20 - 70μm范围内的超薄大面积硅片。基于索-哈钦森力学模型和扭折机制,推导出了一个预测剥落硅片厚度的新方程。为了验证新方程的可靠性,计算了镍在硅片上诱导的应力比例因子。计算得到的比例因子λ = 0.99表明,剥落硅片的厚度与镍层的厚度成正比。在本研究获得的实验数据中也观察到了类似的关系。此外,在使用其他沉积条件和材料时,将应力层的厚度转换为应力值作为参考。剥落了一片预测厚度为50μm的硅片用于进一步分析。为了在不产生切口损失的情况下剥落大面积(150×150mm或6×6英寸)的硅片,通过激光预处理在剥落的硅片内部适当深度(50μm)处形成初始裂纹,这将边缘斜率(切口损失)的面积从33mm²减小到3mm²。剥落硅片的厚度变化保持在4%以内。此外,我们通过使用剥落的硅片制造太阳能电池来检查其退化的可能性;发现剥落硅片的效率和理想因子分别为14.23%和1.35。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4db6/6339913/61dfc9b3f39a/fchem-06-00600-g0012.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4db6/6339913/7b8e0fa0dbc4/fchem-06-00600-g0001.jpg
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https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4db6/6339913/e1b4307a7b7d/fchem-06-00600-g0005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4db6/6339913/daccfc42ab36/fchem-06-00600-g0006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4db6/6339913/4538e43319a5/fchem-06-00600-g0007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4db6/6339913/c9d303c9c183/fchem-06-00600-g0008.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4db6/6339913/8e0236abf6e8/fchem-06-00600-g0009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4db6/6339913/d8d2a55db848/fchem-06-00600-g0010.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4db6/6339913/5b71c96d11a2/fchem-06-00600-g0011.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4db6/6339913/61dfc9b3f39a/fchem-06-00600-g0012.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4db6/6339913/7b8e0fa0dbc4/fchem-06-00600-g0001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4db6/6339913/181b80b0e5d1/fchem-06-00600-g0002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4db6/6339913/dcb9e1944cc9/fchem-06-00600-g0003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4db6/6339913/9dd63f0337a7/fchem-06-00600-g0004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4db6/6339913/e1b4307a7b7d/fchem-06-00600-g0005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4db6/6339913/daccfc42ab36/fchem-06-00600-g0006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4db6/6339913/4538e43319a5/fchem-06-00600-g0007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4db6/6339913/c9d303c9c183/fchem-06-00600-g0008.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4db6/6339913/8e0236abf6e8/fchem-06-00600-g0009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4db6/6339913/d8d2a55db848/fchem-06-00600-g0010.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4db6/6339913/5b71c96d11a2/fchem-06-00600-g0011.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4db6/6339913/61dfc9b3f39a/fchem-06-00600-g0012.jpg

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