4.6 Article

Quantifying the Energy Losses in CsPbI2Br Perovskite Solar Cells with an Open-Circuit Voltage of up to 1.45 V

Journal

ACS ENERGY LETTERS
Volume 7, Issue 11, Pages 4071-4080

Publisher

AMER CHEMICAL SOC
DOI: 10.1021/acsenergylett.2c01883

Keywords

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Funding

  1. China Scholarship Council (CSC)
  2. Erlangen Graduate School in Advanced Optical Technologies (SAOT)
  3. Deutsche Forschungsgemeinschaft (DFG, German Research Foundation) [182849149-SFB 953, INST 90/917, INST 90/1093-1]
  4. Aufbruch Bayern initiative of the state of Bavaria (EnCN and SFF)
  5. Bavarian Initiative Solar Technologies go Hybrid'' (SolTech)
  6. Bavarian State Government [446521a/20/4]

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CsPbI2Br perovskite solar cells show potential as a top cell for tandem applications, but the open-circuit voltage (V-OC) reported so far is usually below the detailed balance (DB) limit for single-junction PSCs. By adding lead acetate to the CsPbI2Br precursor, losses due to nonradiative recombination can be significantly reduced, leading to improved power conversion efficiency and higher V-OC values.
CsPbI2Br perovskite solar cells (PSCs) have attracted much interest because of their thermodynamic stability, relatively stable cubic perovskite phase, and their potential as a top cell for tandem applications. However, the open-circuit voltage (V-OC) reported to date is in most cases well below the detailed balance (DB) limit for single-junction PSCs. Here, we demonstrate that adding lead acetate to the CsPbI2Br precursor allows us to substantially reduce losses due to nonradiative recombination. Corresponding champion devices reach a power conversion efficiency (eta) of 16.7% and a highest V-OC value of 1.45 V, which represents 90% of the DB limit for single-junction PSCs at a bandgap of 1.89 eV. In order to disentangle the nonradiative recombination loss mechanisms, we quantify the origin of energy losses by calculating the radiative limit of the open-circuit voltage (V-OC(rad)) and the quasi-Fermi level splitting (QFLS) of perovskite films with and without other functional layers. We further analyze the strategies to reduce the residual losses in order to push the efficiency beyond the 90% theoretical limit.

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