4.8 Article

Excited States and Their Dynamics in CdSe Quantum Dots Studied by Two-Color 2D Spectroscopy

Journal

JOURNAL OF PHYSICAL CHEMISTRY LETTERS
Volume 13, Issue 5, Pages 1266-1271

Publisher

AMER CHEMICAL SOC
DOI: 10.1021/acs.jpclett.1c04110

Keywords

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Funding

  1. Swedish Research Council (VR)
  2. China Scholarship Council
  3. NanoLund
  4. Knut and Alice Wallenberg Foundation [2016.0089]
  5. Independent Research Fund Denmark-Sapere Aude starting grant [7026-00037A]
  6. Crafoord Foundation [20200522]
  7. Research Fund for International Young Scientists from NSFC, China [21950410515]
  8. Swedish Energy Agency
  9. ADONIS project of the European Regional Development Fund [CZ.02.1.01/0.0/0.0/16_019/0000789]
  10. Ministry of Education, Youth and Sports of the Czech Republic
  11. European Union [945378]
  12. Marie Curie Actions (MSCA) [945378] Funding Source: Marie Curie Actions (MSCA)

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The excited-state dynamics in CdSe QDs were investigated using two-color 2D electronic spectroscopy. It was found that the relaxation of high-energy electrons occurs with a time constant of 100 fs, while the states at the band edge rise within 700 fs. The excited-state absorption also rises with a similar time constant of 700 fs. This study challenges the previous interpretation of the excited-state absorption.
Quantum dots (QDs) form a promising family of nanomaterials for various applications in optoelectronics. Understanding the details of the excited-state dynamics in QDs is vital for optimizing their function. We apply two-color 2D electronic spectroscopy to investigate CdSe QDs at 77 K within a broad spectral range. Analysis of the electronic dynamics during the population time allows us to identify the details of the excitation pathways. The initially excited high-energy electrons relax with the time constant of 100 fs. Simultaneously, the states at the band edge rise within 700 fs. Remarkably, the excited-state absorption is rising with a very similar time constant of 700 fs. This makes us reconsider the earlier interpretation of the excited-state absorption as the signature of a long-lived trap state. Instead, we propose that this signal originates from the excitation of the electrons that have arrived in the conduction-band edge.

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