Abstract

In this contribution, the effectiveness of an RbF post deposition treatment (PDT) is evaluated in dependence on the Cu content of the absorber layer of Cu(In,Ga)Se $_{2}$ solar cells. It is shown that the PDT only acts beneficially on the open-circuit voltage and fill factor ( FF ) on samples with rather high Cu content, while it deteriorates all parameters of the solar cells in samples with low Cu content. In order to clarify the behavior of the open-circuit voltage, the well-known exchange mechanism of Rb and Na during the PDT is analyzed as a function of the Cu content of the absorber layers and discussed in regard to theoretical publications. Furthermore, a model explaining the observed effect on the FF based on the formation of an RbInSe $_{2}$ (RIS) layer during the RbF-PDT is proposed. The model supposes that the RIS layer acts as a barrier for the photocurrent and therefore lowers the FF . It is evaluated theoretically in dependence of the properties of the RIS layer using one-dimensional solar cell capacitance simulator (SCAPS) simulations. Finally, the proposed model is also tested and confirmed experimentally by directly depositing RIS onto untreated Cu(In,Ga)Se $_{2}$ layers.

Highlights

  • I N RECENT years, the implementation of heavy alkali post deposition treatments (PDTs) into the deposition procedure of thin film solar cells based on Cu(In,Ga)Se2 (CIGS) absorber layers has led to significant improvements of the power conversion efficiency (η) of this type of solar cells [1]–[3]

  • Contrary to the results published by Lepetit et al we find that the RbF-PDT only improves all device parameters on samples grown close to stoichiometry, whereas on samples with low CGI all device parameters are decreased

  • We propose a model explaining the observed trends based on device simulations. To test this model, which attributes the observed trend in fill factor (FF) to the formation of RbInSe2 (RIS) at the surface of the CIGS during the PDT, we evaluate the effect of a direct coevaporation of RIS on top of CIGS with CGI = 0.95

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Summary

INTRODUCTION

I N RECENT years, the implementation of heavy alkali post deposition treatments (PDTs) into the deposition procedure of thin film solar cells based on Cu(In,Ga)Se2 (CIGS) absorber layers has led to significant improvements of the power conversion efficiency (η) of this type of solar cells [1]–[3]. The improvement of η of a device due to a PDT is mostly attributed to a gain in open circuit voltage (VOC) and the opportunity to decrease the thickness of the buffer layer resulting in enhanced short-circuit current density (jSC) [1]. Both gain and loss in fill factor (FF) due to the PDTs have been reported [1]–[5].

EXPERIMENTAL
Effects on VOC
Effects on FF
TESTING THE RIS MODEL EXPERIMENTALLY
CONCLUSION

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