相关实验视频

Updated: Jun 21, 2025

Fabrication of Robust Nanoscale Contact between a Silver Nanowire Electrode and CdS Buffer Layer in CuIn,GaSe2 Thin-film Solar Cells

Fabrication of Robust Nanoscale Contact between a Silver Nanowire Electrode and CdS Buffer Layer in CuIn,GaSe2 Thin-film Solar Cells

Published on: July 19, 2019

可扩展的CIGS太阳能电池采用无毒缓冲层和微电网电极的新设备设计

Inchan Hwang¹, Myounghyun Lee², Ahreum Lee¹

¹Photovoltaics Research Department, Korea Institute of Energy Research, Daejeon 34129, Republic of Korea.

ACS applied materials & interfaces

|July 16, 2024

概括

高效,大面积的铜化 (CIGS) 太阳能电池是使用一种新的微电网/透明导电氧化物 (TCO) 混合电极和氧化 (ZMO) 缓冲器开发的. 这种方法克服了TCO的局限性,达到高达20.5%的效率.

科学领域:

材料科学材料科学材料科学
可再生能源可再生能源是可再生能源.
太阳能光伏发电是如何实现的

背景情况:

透明导电氧化物 (TCOs) 由于电气性能差,限制了大面积铜化 (CIGS) 太阳能电池的效率.
开发具有高传导率和导电性的新型顶部电极对于高效,大面积的CIGS设备至关重要.

研究的目的:

设计一个微电网/TCO混合电极,以尽量减少CIGS太阳能电池中的光学和电阻损失.
通过用干燥加工的ZnMgO (ZMO) 缓冲器取代传统的CdS缓冲器来提高设备的效率,减少短波长寄生虫吸收.

主要方法:

制造用于CIGS太阳能电池的微电网/TCO混合电极.
干燥加工的宽带间隙ZnMgO (ZMO) 缓冲层的实施.
优化ZMO缓冲器和微电网/TCO电极组合的优化.

主要成果:

一个小的设备面积 (5毫米×5毫米) 通过反射层实现了20.5%的最大效率.
大面积的CIGS太阳能电池 (20毫米×70毫米) 在微电网/TCO混合电极和反射层上达到19.7%的效率.

结论:

这项研究表明了微电网电极在实现高效率,大面积CIGS太阳能电池方面的潜力.
微电网/TCO混合电极和ZMO缓冲器的组合显著提高了CIGS太阳能电池的性能和可扩展性.

关键词:

这就是CIGS太阳能电池.没有CD的CD.电极设计电极设计大面积的大面积大面积微电网电极电极是微电网的电极.

更多相关视频

In Situ Monitoring of the Accelerated Performance Degradation of Solar Cells and Modules: A Case Study for CuIn,GaSe2 Solar Cells

In Situ Monitoring of the Accelerated Performance Degradation of Solar Cells and Modules: A Case Study for CuIn,GaSe2 Solar Cells

Published on: October 3, 2018

Ambient Method for the Production of an Ionically Gated Carbon Nanotube Common Cathode in Tandem Organic Solar Cells

Ambient Method for the Production of an Ionically Gated Carbon Nanotube Common Cathode in Tandem Organic Solar Cells

Published on: November 5, 2014

相关概念视频

P-N junction

P-N junction

A p-n junction is formed when p-type and n-type semiconductor materials are joined together. At the interface of the p-n junction, holes from the p-side and electrons from the n-side begin to diffuse into the opposite sides due to the concentration gradient. This diffusion of carriers leads to a region around the junction where there are no free charge carriers, known as the depletion region. The charge density within the depletion region for the n-side and p-side can be described by the...