Wet sandblasting pretreatment of diamond wire sawn multi-crystalline silicon wafer for surface acid texturization in photovoltaics

Author(s):  
Runtao Liu ◽  
Yufei Gao ◽  
Chunfeng Yang
Micromachines ◽  
2021 ◽  
Vol 12 (4) ◽  
pp. 429
Author(s):  
Tengyun Liu ◽  
Peiqi Ge ◽  
Wenbo Bi

Lower warp is required for the single crystal silicon wafers sawn by a fixed diamond wire saw with the thinness of a silicon wafer. The residual stress in the surface layer of the silicon wafer is the primary reason for warp, which is generated by the phase transitions, elastic-plastic deformation, and non-uniform distribution of thermal energy during wire sawing. In this paper, an experiment of multi-wire sawing single crystal silicon is carried out, and the Raman spectra technique is used to detect the phase transitions and residual stress in the surface layer of the silicon wafers. Three different wire speeds are used to study the effect of wire speed on phase transition and residual stress of the silicon wafers. The experimental results indicate that amorphous silicon is generated during resin bonded diamond wire sawing, of which the Raman peaks are at 178.9 cm−1 and 468.5 cm−1. The ratio of the amorphous silicon surface area and the surface area of a single crystal silicon, and the depth of amorphous silicon layer increases with the increasing of wire speed. This indicates that more amorphous silicon is generated. There is both compressive stress and tensile stress on the surface layer of the silicon wafer. The residual tensile stress is between 0 and 200 MPa, and the compressive stress is between 0 and 300 MPa for the experimental results of this paper. Moreover, the residual stress increases with the increase of wire speed, indicating more amorphous silicon generated as well.


2007 ◽  
Vol 46 (1) ◽  
pp. 21-23 ◽  
Author(s):  
Norihito Kawaguchi ◽  
Ryusuke Kawakami ◽  
Ken-ichiro Nishida ◽  
Naoya Yamamoto ◽  
Miyuki Masaki ◽  
...  

2016 ◽  
Vol 120 (23) ◽  
pp. 235308 ◽  
Author(s):  
Anass Benayad ◽  
Hamza Hajjaji ◽  
Fabrice Coustier ◽  
Malek Benmansour ◽  
Amal Chabli

2017 ◽  
Vol 28 (24) ◽  
pp. 18825-18834 ◽  
Author(s):  
Yuxin Zou ◽  
Shaoyuan Li ◽  
Wenhui Ma ◽  
Zhao Ding ◽  
Fengshuo Xi ◽  
...  

2002 ◽  
Vol 719 ◽  
Author(s):  
A.Y. Usenko ◽  
W.N. Carr ◽  
Bo Chen

AbstractFeatures of a process of delamination of crystalline silicon layer from silicon wafer along hydrogen platelet layer formed by microwave plasma hydrogenation are described. The process involves first making a buried layer of nuclei for hydrogen platelets. Ion implantation of inert or low-soluble gases is used to form the layer. The nuclei are microbubbles that appear along Rp plane of implanted ions. Results for argon, xenon, and krypton implantation are compared. Wafers thus processed with a dose of 1015cm-2 are then hydrogenated with a microwave plasma. During hydrogenation, an atomic hydrogen diffuses into the silicon wafer and collects onto internal surfaces of the microbubbles. Then the hydrogen increases the internal surface of the microbubbles by growing a platelet type extensions to the microbubbles. The extensions grow preferably along the buried layer plane. A silicon layer above the layer of grown platelets were delaminated through pre-bonding/cut/post-bonding sequence as in the Smart-cut process. The plasma hydrogenation of the trap layer may be used as a step in a process of fabricating of SOI wafers with a very thin top crystalline silicon layer. Also, implant doses needed to form the microbubble trap layer are much lower than doses of direct implantation of hydrogen in the Smart-cut process. Temperature range of 200°C to 400°C during the hydrogenation process allows effectively grow extended hydrogen platelets from the nuclei. Mechanisms of nucleation of platelets as extentions of microbubbles are suggested. Control of hydrogen outdiffusion/platelet growth with thermal trajectory during plasma processing is discussed.


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