Abstract

AbstractThe open‐circuit voltage (VOC) is the main limitation to higher efficiencies of Cu(In,Ga)Se2 solar cells. One of the most critical parameters directly affecting VOC is the charge carrier lifetime. Therefore, it is essential to evaluate the extent to which inhomogeneities in material properties limit the carrier lifetime and how postdeposition treatments (PDTs) and growth conditions affect material properties. Time‐resolved photoluminescence (TRPL) microscopy is employed at conditions similar to one sun to study carrier lifetime fluctuations in Cu(In,Ga)Se2 with light (Na) and heavy (Rb) alkalis, different substrates, and grown at different temperatures. PDT lowers the amplitude of minority carrier lifetime fluctuations, especially for Rb‐treated samples. Upon PDT, the grains’ carrier lifetime increases, and the analysis suggests a reduction in grain boundary recombination. Furthermore, lifetime fluctuations have a small impact on device performance, whereas VOC calculated from TRPL (and continuous‐wave PL) agrees with device values within the limits of investigated PDT samples. Finally, up to about half a per cent external radiative efficiencies are experimentally determined from TRPL metrics, and internal radiative efficiencies are approximated. The findings demonstrate that the highest absorber material quality investigated is still limited by nonradiative recombination (grain or grain boundary) and is comparable to state‐of‐the‐art absorbers.

Highlights

  • The five samples investigated include double-graded absorbers grown on soda-lime glass (SLG) and stainless-steel (Steel) at low temperature (LT) and high temperature (HT) with different postdeposition treatments (PDTs) applied: No PDT, NaF, and NaF + RbF

  • We have shown PDT homogenizes spatial variations of carrier lifetime and overall PL intensity, with RbF and NaFtreated samples exhibiting lower spatial variations compared to No-PDT

  • The maximum deviations from the mean in Time-resolved photoluminescence (TRPL) parameters are within ±20% and for the No-PDT sample ±40%

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Summary

Results and Discussion

The five samples investigated include double-graded absorbers grown on soda-lime glass (SLG) and stainless-steel (Steel) at low temperature (LT) and high temperature (HT) with different PDT applied: No PDT, NaF, and NaF + RbF (see the Experimental Section for more details about the samples). For TRPL mapping, solar cells of layer structure CdS/CIGS/Mo were used after etching away ZnO layers to access the same region where conventional photovoltaic (PV) characterization was performed. As previously shown by Metzger et al.[18] and suggested by Weiss et al.,[19] the presence of CdS has a minor or null impact on the TRPL decay, which applies to the samples studied here. The solar cells investigated exhibit a significant difference in performance, as shown by the I–V parameters of Table 1

TRPL Mapping under Wide-Field Illumination
Grain Boundary Recombination
TRPL Power Dependence and Injection Conditions
VOC Loss Analysis from Steady-State PL and TRPL Parameters
Conclusions
Experimental Section
Data Availability Statement
Full Text
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