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Borosiloxane boron diffusion for p-emitter formation on n-type silicon wafers

机译:硼硅氧烷硼扩散用于在n型硅晶片上形成p发射极

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摘要

Thermal boron diffusion, which forms highly doped and shallow p-emitters on phosphor-doped silicon wafers, is one of the primary processes in commercial-scale production of n-type cells. Here, we report on the use of nontoxic and nonvolatile borosiloxane sols as the spin-on boron source. In comparison to the tribromide (BBr_3) boron diffusion that is applied in the production of most commercial n-type cells, borosiloxane boron diffusion may have potential advantages in terms of cost, safety, operability, etc. The borosiloxane sols studied here were formed from a cross-linking reaction between boron acid and a mixture of two types of silicon alkoxides, methyltriethoxysilane (MTEOS) and dimethyldiethoxysilane (DMDEOS). The MTEOS/DMDEOS ratio was found to be the key factor determining the synthetic period, net structure, thermal transformation property, and coating behavior of the borosiloxane sols. In combination with the spin-coating method, the performance of borosiloxane boron diffusion into phosphor-doped silicon wafers (1-3 Ω·cm) was systematically investigated by varying the borosiloxane composition (boron/silicon or MTEOS/DMDEOS ratio) and the diffusion process parameters (temperature, ambience, and period of individual sub-steps), and by relating them to the resulting sheet resistance and boron doping profile. The results show that under the diffusion conditions in conventional cell production lines, the formed p-emitters can have variable sheet resistance in the range of 35-582 Ω/□ and boron doping depth of 100-300 nm.
机译:硼的热扩散会在掺磷的硅片上形成高度掺杂的浅p型发射极,是n型电池商业规模生产的主要工艺之一。在这里,我们报道了无毒,不挥发的硼硅氧烷溶胶作为旋涂硼源的使用。与大多数商用n型电池生产中使用的三溴化物(BBr_3)硼扩散相比,硼硅氧烷硼扩散在成本,安全性,可操作性等方面可能具有潜在的优势。此处研究的硼硅氧烷溶胶是由硼酸与两种类型的硅醇盐(甲​​基三乙氧基硅烷(MTEOS)和二甲基二乙氧基硅烷(DMDEOS))的混合物之间的交联反应。发现MTEOS / DMDEOS之比是决定硼硅氧烷溶胶的合成周期,净结构,热转化性能和涂覆行为的关键因素。结合旋涂法,通过改变硼硅氧烷的组成(硼/硅或MTEOS / DMDEOS的比例)和扩散,系统地研究了硼硅氧烷硼扩散到掺磷的硅片(1-3Ω·cm)中的性能。工艺参数(温度,环境温度和各个子步骤的周期),并将它们与所得的薄层电阻和硼掺杂分布相关联。结果表明,在常规电池生产线的扩散条件下,所形成的p型发射极可以具有在35-582Ω/□范围内的可变薄层电阻和100-300nm的硼掺杂深度。

著录项

  • 来源
    《Journal of materials science》 |2017年第16期|11563-11568|共6页
  • 作者单位

    Key Laboratory for Ultrafine Materials of Ministry of Education, School of Materials Science and Engineering, East China University of Science and Technology, Shanghai, China;

    Key Laboratory for Ultrafine Materials of Ministry of Education, School of Materials Science and Engineering, East China University of Science and Technology, Shanghai, China;

    Key Laboratory for Ultrafine Materials of Ministry of Education, School of Materials Science and Engineering, East China University of Science and Technology, Shanghai, China;

    Key Laboratory for Ultrafine Materials of Ministry of Education, School of Materials Science and Engineering, East China University of Science and Technology, Shanghai, China;

    Key Laboratory for Ultrafine Materials of Ministry of Education, School of Materials Science and Engineering, East China University of Science and Technology, Shanghai, China;

    Key Laboratory for Ultrafine Materials of Ministry of Education, School of Materials Science and Engineering, East China University of Science and Technology, Shanghai, China;

    Key Laboratory for Ultrafine Materials of Ministry of Education, School of Materials Science and Engineering, East China University of Science and Technology, Shanghai, China;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
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  • 正文语种 eng
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