非晶溅射ITO薄膜作为能量自主无线微系统CIGS太阳能电池透明前接触层的研究进展

T. Aviles, C. Lethien, M. Zegaoui, J. Vilcot, F. Leroy, P. Roussel, N. Rolland, P. Rolland
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引用次数: 3

摘要

本文报道了室温下射频溅射氧化铟锡(ITO)薄膜的电学、光学和结构性能的研究。这些薄膜专门用作CIGS太阳能微电池的前电极,并且必须符合此类应用所需的电学和光学标准。众所周知,溅射沉积技术的主要缺点是其固有的高能粒子的产生会导致对样品的轰击。开发的沉积工艺的目标是不损坏底层,因为在CIGS太阳能电池的情况下,保持吸收层的表面和特性是至关重要的,这些薄膜将沉积在吸收层上。在室温下,可以认为只有当高能轰击不发生时才能得到非晶ITO薄膜。如果粒子的动能被沉积等离子体内的碰撞完全耗散,就可以得到这一点[1-3]。沉积过程是在传统的磁控溅射系统中进行的,没有外部加热,因此薄膜应该是无定形的。此外,薄膜内应力保持在很低的水平。光学研究表明,在可见光范围内的透明度超过80%,在红外区域的透明度很高。得到的最低薄片电阻为12.6 Ω/□(膜厚约300nm),载流子浓度为2.4 × 1020 cm−3,载流子迁移率为45.1 cm2/V.s。由于我们可以沉积双ITO层结构,每层具有不同的电阻率水平,我们建议我们的非晶ITO薄膜可以直接沉积在吸收CIGS材料的上方,作为高阻(HR)和电极层。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Recent developments in amorphous sputterred ITO thin films acting as transparent front contact layer of CIGS solar cells for energy autonomous wireless microsystems
In this paper, we report on the study of electrical, optical and structural properties of RF sputtered Indium Tin Oxide (ITO) thin films at room temperature. These films are dedicated to act as front electrode of CIGS solar microcells and shall so compel with the electrical and optical criteria that are required for such an application. It is well-known that the main drawback of the sputtering deposition technique deals with the inherent generation of highly energetic particles that causes bombardment onto the sample. The developed deposition process targets to be damage free onto the underlying layer since, in the case of CIGS solar cells, it is crucial to preserve the surface and the properties of the absorber layer on which these films will be deposited. At room temperature, it can be considered that amorphous ITO films are only obtained when this energetic bombardment does not occur. This can be obtained if the kinetic energy of the particles is fully dissipated by collisions within the deposition plasma [1–3]. The deposition process is developed in a conventional magnetron sputtering system without external heating, in such a way that films shall be amorphous. Furthermore, film internal stress is kept very low. Optical studies show a transparency over 80% in the visible range and a high transparency in the infrared region. The lowest obtained sheet resistance is 12.6 Ω/□ (∼ 300nm film thickness) with a carrier concentration of 2.4 × 1020 cm−3 and a carrier mobility of 45.1 cm2/V.s. As we can deposit a dual ITO layer structure, with a different resistivity level being attributed to each layer, we suggest our amorphous ITO thin films can be deposited directly above the absorbing CIGS material to act as both highly resistive (HR) and electrode layer.
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