Revealing the beneficial role of K in grain interiors, grain boundaries, and at the buffer interface for highly efficient CuInSe2 solar cells

Christopher P. Muzzillo, Jonathan D. Poplawsky, Ho Ming Tong, Wei Guo, Tim Anderson

Research output: Contribution to journalArticlepeer-review

19 Scopus citations

Abstract

K incorporation within grain boundaries, grain interiors, and interfaces has been studied within CuInSe2 solar cells to better understand the beneficial or detrimental role of K distribution among these regions in chalcopyrite-based solar cells. Solar cells have been fabricated with intentional K introduction into specific regions of the device including the CuInSe2/CdS interface (CuInSe2/KInSe2/CdS) and the grain interiors (Cu0.93K0.07InSe2/CdS). A control CuInSe2/CdS device was also studied to separate effects of K originating from the soda-lime glass substrate from those of intentionally introduced K. The experiment was designed to understand K effects in Cu(In,Ga)Se2 solar cells while mitigating complications from multiple elements in the 3+ site. The distribution of all elements within these samples has been directly observed with sub-nm resolution via atom probe tomography. In addition, electron beam–induced current measurements have been performed to correlate the atom probe tomography compositional profiles to the nanoscale carrier collection properties. The experiments show that a large decrease in the Cu/In ratio at the CdS interface can be achieved by forming KInSe2 at the absorber surface, which drastically improves the device efficiency. The results presented here show a direct link between K concentration, Cu depletion, and In accumulation, such that the Cu/In ratio significantly reduces with K incorporation. The findings help clarify the mechanism behind K-induced efficiency enhancement.

Original languageEnglish
Pages (from-to)825-834
Number of pages10
JournalProgress in Photovoltaics: Research and Applications
Volume26
Issue number10
DOIs
StatePublished - Oct 2018

Funding

The authors thank Stephen Glynn, Lorelle Mansfield, and Carolyn Beall for assistance with experiments, Clay DeHart for contact deposition, and Karen Bowers for device processing. TEM, APT, and EBIC were performed at the Center for Nanophase Materials Sciences at Oak Ridge National Laboratory, which is a US DOE Office of Science User Facility. The authors thank Karren More for guidance. This work was supported by the US Department of Energy under contract no. DE‐AC36‐08GO28308 with Alliance for Sustainable Energy, LLC, the Manager and Operator of the National Renewable Energy Laboratory. Funding provided by US Department of Energy Office of Energy Efficiency and Renewable Energy Solar Energy Technologies Office. Work was done under the CIGS F‐PACE agreement. The authors thank Stephen Glynn, Lorelle Mansfield, and Carolyn Beall for assistance with experiments, Clay DeHart for contact deposition, and Karen Bowers for device processing. TEM, APT, and EBIC were performed at the Center for Nanophase Materials Sciences at Oak Ridge National Laboratory, which is a US DOE Office of Science User Facility. The authors thank Karren More for guidance. This work was supported by the US Department of Energy under contract no. DE-AC36-08GO28308 with Alliance for Sustainable Energy, LLC, the Manager and Operator of the National Renewable Energy Laboratory. Funding provided by US Department of Energy Office of Energy Efficiency and Renewable Energy Solar Energy Technologies Office. Work was done under the CIGS F-PACE agreement.

FundersFunder number
US Department of Energy
U.S. Department of EnergyDE-AC36-08GO28308

    Keywords

    • Cu(In,Ga)Se
    • CuInSe
    • atom probe tomography
    • chalcopyrite
    • electron beam–induced current
    • potassium

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