4.8 Article

Slow Auger Recombination of Trapped Excitons Enables Efficient Multiple Electron Transfer in CdS-Pt Nanorod Heterostructures

Journal

JOURNAL OF THE AMERICAN CHEMICAL SOCIETY
Volume 143, Issue 48, Pages 20264-20273

Publisher

AMER CHEMICAL SOC
DOI: 10.1021/jacs.1c09125

Keywords

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Funding

  1. U.S. Department of Energy, Office of Science, Office of Basic Energy Sciences, Solar Photochemistry Program [DE-SC0008798]
  2. U.S. Department of Energy (DOE) [DE-SC0008798] Funding Source: U.S. Department of Energy (DOE)

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The study explores the dynamics of multiple electron transfer in CdS-Pt nanorods, revealing the efficiency and competition in multiexciton dissociation and electron transfer processes. This has implications for driving multielectron photocatalytic reactions and controlling product selectivity under intense illumination.
Solar-to-fuel conversion reaction often requires multiple proton-coupled electron transfer (PCET) processes powered by the energetic electrons and/or holes generated by the absorption of multiple photons. The effective coupling of multiple electron transfer from the light absorber with the multiple PCET reactions at the catalytic center is one of the key challenges in efficient and selective conversion of solar energy to chemical fuels. In this paper, we examine the dynamics of multiple electron transfer in quantum confined CdS nanorods with a Pt tip, in which the CdS rod functions as the light absorber and the Pt tip the catalytic center. By excitation-fluence-dependent transient absorption spectroscopic measurements, we show that the multiexciton Auger recombination rate in CdS rods follows a carrier-collision model, k(n)(A) = n(2)(n - 1)/4k(2)(A), with a biexciton lifetime (1/k(2)(A)) of 2.0 +/- 0.2 ns. In CdS-Pt nanorods, electron transfer kinetics from the CdS conduction band edge to the Pt show negligible dependence on the excitation fluence, occurring with a half-life time of 5.6 +/- 0.6 ps. The efficiency of multiple exciton dissociation by multiple electron transfer to Pt decreases from 100% in biexciton states to similar to 41% at 22 exciton state due to the competition with Auger recombination. The half-lifetime of the n-charge separated state recombination (with n electrons in the Pt and n holes in the CdS) decreases from 10 mu s in the single charge separated state to 42 ns in nine charge separated states. Our findings suggest the possibility of driving multielectron photocatalytic reactions under intense illumination and controlling product selectivity through multielectron transfer.

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