Abstract

This review summarizes all studies which used dielectric-based materials as a passivation layer at the rear surface of copper indium gallium (di)selenide, Cu(In,Ga)Se2, (CIGS)-based thin film solar cells, up to 2019. The results regarding the kind of dielectric materials, the deposition techniques, contacting approaches, the existence of additional treatments, and current–voltage characteristics (J–V) of passivated devices are emphasized by a detailed table. The techniques used to implement the passivation layer, the contacting approach for the realization of the current flow between rear contact and absorber layer, additional light management techniques if applicable, the solar simulator results, and further characterization techniques, i.e., external quantum efficiency (EQE) and photoluminescence (PL), are shared and discussed. Three graphs show the difference between the reference and passivated devices in terms of open-circuit voltage (Voc), short-circuit current (Jsc), and efficiency (η), with respect to the thicknesses of the absorber layer. The effects of the passivation layer at the rear surface are discussed based on these three graphs. Furthermore, an additional section is dedicated to the theoretical aspects of the passivation mechanism.

Highlights

  • The energy coming from the sun has the highest potential energy of all renewable resources, and it is ~35,000 times higher than today’s energy needs on a yearly basis

  • This review summarizes all studies which used dielectric-based materials as a passivation layer at the rear surface of copper indium galliumselenide, Cu(In,Ga)Se2, (CIGS)-based thin film solar cells, up to 2019

  • The effects of the passivation mechanism are more observable for thinner CIGS absorber layers, as explained earlier

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Summary

Introduction

The energy coming from the sun has the highest potential energy of all renewable resources, and it is ~35,000 times higher than today’s energy needs on a yearly basis. The production step starts with a sputtering molybdenum (Mo) layer as an electrical back contact on soda-lime glass (SLG), metal, or polymer substrate It is continued with the p-type CIGS absorber layer deposition by using co-evaporation, sputtering, or electro-deposition techniques. If the thickness of the layer absorber layer is decreased, the quality electrical of these the power conversion efficiency, should be kept the same or, if possible, improved. Ga layers grading is Ga not and the BSF is created in theregion space (SCR), charge improving region (SCR), Voc for layers thin absorber [6]. Introducing a passivation layer and improved solution passivate rear surface of CIGS In this In paper, overview of the papers usethat this absorber layer is oneto ofthis the problem solutions(Figure to this 2).

Theoretical Aspects
Dielectric-Based Passivation Layers
Transmission
Approaches Used to Add the Passivation Layer
Contacting Approach
Solar Simulator Results
Other Characterization Techniques for Further Characterizations
Conclusions
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