Millisecond‐Scale Charge‐Carrier Recombination Dynamics in the CsPbBr3 Perovskite

Author:

Bojtor András12ORCID,Krisztián Dávid12,Korsós Ferenc2,Kollarics Sándor134,Paráda Gábor2ORCID,Pinel Thomas15,Kollár Márton6ORCID,Horváth Endre6,Mettan Xavier6,Shiozawa Hidetsugu78,Márkus Bence G.139ORCID,Forró László9,Simon Ferenc134ORCID

Affiliation:

1. Department of Physics Institute of Physics Budapest University of Technology and Economics Műegyetem rkp. 3 H‐1111 Budapest Hungary

2. Semilab Co. Ltd. Prielle Kornélia u. 2 1117 Budapest Hungary

3. Institute for Solid State Physics and Optics HUN‐REN Wigner Research Centre for Physics PO. Box 49 H‐1525 Budapest Hungary

4. ELKH‐BME Condensed Matter Research Group Budapest University of Technology and Economics Műegyetem rkp. 3 1111 Budapest Hungary

5. Engineering physics and embedded systems École Nationale Supérieure d'ingénieurs de Caen 6 Bd Maréchal Juin 14000 Caen France

6. Research and Development Department KEP Innovation Center Ch. du Pré‐Fleuri 5 1228 Plan‐les‐Ouates Switzerland

7. J. Heyrovsky Institute of Physical Chemistry Czech Academy of Sciences Dolejškova 182 23 Prague 8 Czech Republic

8. Faculty of Physics University of Vienna Boltzmanngasse 5 1090 Vienna Austria

9. Stavropoulos Center for Complex Quantum Matter Department of Physics and Astronomy University of Notre Dame Notre Dame 46556 IN USA

Abstract

Understanding the recombination lifetime of charge carriers () is essential for the diverse applications of photovoltaic materials, such as perovskites. The study on the inorganic perovskite, CsPbBr3, reveals recombination dynamics exceeding 1 ms below 200 K and approaching 100 μs at room temperature. Utilizing time‐resolved microwave‐detected photoconductivity decay in conjunction with injection dependence, it is found that is dominated by impurity charge trapping. The observed injection dependence is well corroborated by modeling of the trap mechanism. The ultralong decay time is also consistent with photoconductivity measurements with a continuous‐wave excitation at powers corresponding to around 1 Sun irradiation. While charge‐carrier trapping may, in theory, impose limitations on the photovoltaic efficiency of single‐cell devices, it can also contribute to increased efficiency in tandem cells and find applications in photodetection, photocatalysis, and quantum information storage.

Funder

National Research, Development and Innovation Office

Grantová Agentura České Republiky

Ministerstvo Školství, Mládeže a Tělovýchovy

Publisher

Wiley

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