Abstract

$\mathrm{Cu}(\mathrm{In},\mathrm{Ga}){\mathrm{S}}_{2}$ is a promising semiconductor that offers excellent prospects for photovoltaics. However, the performance has been plagued mostly due to large photovoltage deficit. Here, we investigate defects and optoelectronic properties of 1.7-eV band gap near-stoichiometric $\mathrm{Cu}(\mathrm{In},\mathrm{Ga}){\mathrm{S}}_{2}$ (CIGS). We have estimated quasi-Fermi-level splitting of 921 meV from steady state photoluminescence (PL) measurements at 1 sun. Detailed analysis of temperature and excitation dependent PL reveals the behavior of a strongly compensated semiconductor. We show that spatially varying energetic disorder, described by electrostatic potential fluctuations, causes band-tail recombination and strongly affects the carrier recombination in compensated CIGS. Apart from band-tail transitions, we also observe two deep defects at about 0.3 and 0.45 eV below the band edge. The defects are also discerned by admittance measurements. Temperature dependent current-voltage measurements show that the open-circuit voltage is further limited by interface recombination. Thus, the performance improvement lies in the mitigation of deep defect states and absorber/buffer interface optimization.

Highlights

  • The field of photovoltaics (PV) has witnessed considerable advancements in the past few decades leading to material innovations, advanced engineering, and improved fundamental understanding

  • Structural characterization was performed by X-ray diffraction (XRD) analysis of polycrystalline CIGS thin films

  • We present a detailed analysis of recombination processes in 1.7-eV band gap CIGS

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Summary

INTRODUCTION

The field of photovoltaics (PV) has witnessed considerable advancements in the past few decades leading to material innovations, advanced engineering, and improved fundamental understanding. Proposed explanations include the existence of phase impurities [16,17], conducting Cu-S related phases [18], recombination losses due to high concentration of intrinsic bulk point defects ( extended defect states due to sulfur vacancies and cation antisite defects) [15,19], back surface recombination at Mo and absorber/buffer interface (front surface) [20,21,22,23] This indicates that the key to higher QFLS, and Voc, lies in mitigating the defects and improving the optoelectronic quality of. We suggest the origin of tail states due to electrostatic potential fluctuations arising from random spatial variations in defect density These fluctuations influence the PL transition which are identified in terms of energy shift of the PL maximum with excitation and temperature. III, additional characterization results are provided in the Supplemental Material [37]

EXPERIMENTAL DETAILS
Structural characterization and phase analysis
Photoluminescence and defect analysis
Device performance and analysis
CONCLUSION
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