The Role of Oxygen Exposure on the Performance of All-Vapor-Processed Perovskite Solar Cells With CuPC Hole Transport Layers

Methylammonium lead iodide (MAPbI<sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">3</sub>) perovskite solar cells were made using an all-vapor process, including two-step close space vapor transport-processed MAPbI<sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">3</sub> absorber and evaporated copper phthalocyanine (CuPC) hole transport layer (HTL). N-i-p solar cells fabricated entirely in a nitrogen glovebox had poor performance due to s-shaped J-V curves and fill factors (FF) <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><tex-math notation="LaTeX">$&lt; $</tex-math></inline-formula>45%. Solar cells exposed to dry air in a desiccator for seven days, or to O<sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sub> flowed into the evaporator during CuPC deposition, had significantly improved performance with reduced or eliminated s-shaped behavior and improved FF up to 72%. Co-planar conductivity measurements show that exposure to dry air, deposition with oxygen, and MoO<sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">x</sub> capping layers all increase the conductivity of the CuPC HTL. Drift-diffusion simulations show that increasing hole concentration consistent with oxygen doping effects can explain the J-V behavior of the solar cell. Solar cells using spiro-OMeTAD HTLs achieved similar Power Conversion Efficiency but higher V<sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">oc</sub> up to 1.01 V. Drift-diffusion simulations show that the V<sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">oc</sub> difference can be explained by differences in doping density and valence band position between spiro and CuPC.

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Publication Details

Journal
IEEE Journal of Photovoltaics
Published
2024-08-15
DOI
https://doi.org/10.1109/jphotov.2024.3414125
Citations
7
Primary Topic
Perovskite Materials and Applications
Type
article
Field-Weighted Citation Impact
1.46

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article

The Role of Oxygen Exposure on the Performance of All-Vapor-Processed Perovskite Solar Cells With CuPC Hole Transport Layers

William N. Shafarman, Ujjwal Das, Kevin D. Dobson, Austin G. Kuba et al.
7 citations
IEEE Journal of Photovoltaics
Perovskite Materials and Applications
1.46
article

The Role of Oxygen Exposure on the Performance of All-Vapor-Processed Perovskite Solar Cells With CuPC Hole Transport Layers

William N. Shafarman, Ujjwal Das, Kevin D. Dobson, Austin G. Kuba, Alexander J. Harding, Brian E. McCandless, Bin Du
article en
7 citations

Abstract

Methylammonium lead iodide (MAPbI<sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">3</sub>) perovskite solar cells were made using an all-vapor process, including two-step close space vapor transport-processed MAPbI<sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">3</sub> absorber and evaporated copper phthalocyanine (CuPC) hole transport layer (HTL). N-i-p solar cells fabricated entirely in a nitrogen glovebox had poor performance due to s-shaped J-V curves and fill factors (FF) <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><tex-math notation="LaTeX">$&lt; $</tex-math></inline-formula>45%. Solar cells exposed to dry air in a desiccator for seven days, or to O<sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sub> flowed into the evaporator during CuPC deposition, had significantly improved performance with reduced or eliminated s-shaped behavior and improved FF up to 72%. Co-planar conductivity measurements show that exposure to dry air, deposition with oxygen, and MoO<sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">x</sub> capping layers all increase the conductivity of the CuPC HTL. Drift-diffusion simulations show that increasing hole concentration consistent with oxygen doping effects can explain the J-V behavior of the solar cell. Solar cells using spiro-OMeTAD HTLs achieved similar Power Conversion Efficiency but higher V<sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">oc</sub> up to 1.01 V. Drift-diffusion simulations show that the V<sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">oc</sub> difference can be explained by differences in doping density and valence band position between spiro and CuPC.

IEEE Journal of PhotovoltaicsVol. 14(5)
University of Delaware (US)
National Science Foundation
Openalex Percentile: Top 18%
Perovskite Materials and Applications
1.46
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