4.8 Article

Biexciton Binding Energy and Line width of Single Quantum Dots at Room Temperature

Journal

NANO LETTERS
Volume 21, Issue 13, Pages 5760-5766

Publisher

AMER CHEMICAL SOC
DOI: 10.1021/acs.nanolett.1c01556

Keywords

quantum dots; single-quantum-dot spectroscopy; multiexciton emission; biexciton line width

Funding

  1. Dutch Research Council NWO [OCENW.KLEIN.008]
  2. Netherlands Organisation for Scientific Research NWO [722.017.002]
  3. Netherlands Center for Multiscale Catalytic Energy Conversion (MCEC)
  4. European Research Council Horizon 2020 ERC [678004]
  5. European Research Council (ERC
  6. FP/2007-2013) [339905]

Ask authors/readers for more resources

A novel spectroscopic method, cascade spectroscopy, was used to quantify the biexciton line width and binding energy of single CdSe/CdS/ZnS colloidal quantum dots at room temperature. The average emission line width of biexcitons was found to be 86 meV, similar to that of excitons, with variations in biexciton repulsion more narrowly distributed than variations in exciton energy. Inhomogeneous broadening in the sample was primarily attributed to variations in the CdS shell thickness.
Broadening of multiexciton emission from colloidal quantum dots (QDs) at room temperature is important for their use in high-power applications, but an in-depth characterization has not been possible until now. We present and apply a novel spectroscopic method to quantify the biexciton line width and biexciton binding energy of single CdSe/CdS/ZnS colloidal QDs at room temperature. In our method, which we term cascade spectroscopy, we select emission events from the biexciton cascade and reconstruct their spectrum. The biexciton has an average emission line width of 86 meV on the single-QD scale, similar to that of the exciton. Variations in the biexciton repulsion (E-b = 4.0 +/- 3.1 meV; mean +/- standard deviation of 15 QDs) are correlated with but are more narrowly distributed than variations in the exciton energy (10.0 meV standard deviation). Using a simple quantum-mechanical model, we conclude that inhomogeneous broadening in our sample is primarily due to variations in the CdS shell thickness.

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