Abstract

Despite the potential in single- and multi-junction solar cells application, research into the wide band gap CuIn1−xGax(Se1−ySy)2 or CIG(SSe)2 solar cell material, with Eg≥1.5eV, has yet to be extensively performed to date. In this work, we conducted a numerical study into the role of the n-type layers in CIG(SSe)2 heterojunction solar cells, specifically concerning the maximum open-circuit voltage of the devices. In the first part of the study, we derived a new ideal open-circuit voltage equation for a thin-film heterojunction solar cell by taking into account the current contribution from the depletion region. The accuracy of the new equation was validated through a simulation model in the second part of the study. Another simulation model was also used to clarify the design rules of the n-type layer in a wide band gap CIG(SSe)2 solar cell. Our work stressed the importance of a positive conduction band offset on the n-/p-type interface, through the use of a low electron affinity n-type material for a solar cell with a high open-circuit voltage. Through a precise selection of the window layer material, a buffer-free CIG(SSe)2 design is sufficient to fulfill such conditions. We also proposed the specific roles of the n-type layer, i.e., as a passivation layer and selective electron contact, in the operation of CIGS2 solar cells.

Highlights

  • Chalcopyrite CuIn1− x Gax (Se1−y Sy )2 or CIG(SSe)2 solar cells are one of the prominent materials used in the thin-film solar cell technology

  • In the second part of the study, we focused on analysing the effect of the n-type layer materials on the open-circuit voltage of the ideal band gap CIGS2 solar cell devices

  • Wide band gap CIG(SSe)2 has the potential to be a top cell for tandem solar cell applications

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Summary

Introduction

Chalcopyrite CuIn1− x Gax (Se1−y Sy ) or CIG(SSe) solar cells are one of the prominent materials used in the thin-film solar cell technology. The application of alternative n-type materials, such as ZnO1− x Sx :Al [32] or Zn1− x Mgx O:Al [33], on a buffer-free CIG(SSe) absorber layer has been shown to be advantageous on the solar cell performance. In both papers, the authors argued that the improved solar cell characteristics were due to the conduction band’s offset alignment on the pn-junction interface. In the second part of the study, we focused on analysing the effect of the n-type layer materials on the open-circuit voltage of the ideal band gap CIGS2 solar cell devices

Theoretical-VOC Equation
N-Type Layer Simulation Modelling
Maximum VOC and Band Diagram Analysis in Ideal Design Condition
The Roles of N-Type Layer in Realistic Design Condition
N-Type Layer as Interface Passivation
N-Type Layer as Selective Electron Contact
Conclusions
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