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Ultrafast Exciton Dynamics of CH3NH3PbBr3 Perovskite Nanoclusters.
Cherrette, Vivien L; Chou, Kai-Chun; Zeitz, David; Guarino-Hotz, Melissa; Khvichia, Mariam; Barnett, Jeremey; Win, Allison; Babbe, Finn; Zhang, Jin Z.
Afiliação
  • Cherrette VL; Department of Chemistry and Biochemistry, University of California, Santa Cruz, California 95064, United States.
  • Chou KC; Department of Chemistry and Biochemistry, University of California, Santa Cruz, California 95064, United States.
  • Zeitz D; Department of Chemistry and Biochemistry, University of California, Santa Cruz, California 95064, United States.
  • Guarino-Hotz M; Department of Chemistry and Biochemistry, University of California, Santa Cruz, California 95064, United States.
  • Khvichia M; Department of Chemistry and Biochemistry, University of California, Santa Cruz, California 95064, United States.
  • Barnett J; Department of Chemistry and Biochemistry, University of California, Santa Cruz, California 95064, United States.
  • Win A; Department of Chemistry and Biochemistry, University of California, Santa Cruz, California 95064, United States.
  • Babbe F; Chemical Science Division, Lawrence Berkeley National Laboratory, Berkeley, California 94720, United States.
  • Zhang JZ; Department of Chemistry and Biochemistry, University of California, Santa Cruz, California 95064, United States.
J Phys Chem Lett ; 15(19): 5177-5182, 2024 May 16.
Article em En | MEDLINE | ID: mdl-38717311
ABSTRACT
Exciton dynamics of perovskite nanoclusters has been investigated for the first time using femtosecond transient absorption (TA) and time-resolved photoluminescence (TRPL) spectroscopy. The TA results show two photoinduced absorption signals at 420 and 461 nm and a photoinduced bleach (PB) signal at 448 nm. The analysis of the PB recovery kinetic decay and kinetic model uncovered multiple processes contributing to electron-hole recombination. The fast component (∼8 ps) is attributed to vibrational relaxation within the initial excited state, and the medium component (∼60 ps) is attributed to shallow carrier trapping. The slow component is attributed to deep carrier trapping from the initial conduction band edge (∼666 ps) and the shallow trap state (∼40 ps). The TRPL reveals longer time dynamics, with modeled lifetimes of 6.6 and 93 ns attributed to recombination through the deep trap state and direct band edge recombination, respectively. The significant role of exciton trapping processes in the dynamics indicates that these highly confined nanoclusters have defect-rich surfaces.

Texto completo: 1 Coleções: 01-internacional Base de dados: MEDLINE Idioma: En Revista: J Phys Chem Lett Ano de publicação: 2024 Tipo de documento: Article

Texto completo: 1 Coleções: 01-internacional Base de dados: MEDLINE Idioma: En Revista: J Phys Chem Lett Ano de publicação: 2024 Tipo de documento: Article