4.8 Article

Identification of Two Regimes of Carrier Thermalization in PbS Nanocrystal Assemblies

Journal

JOURNAL OF PHYSICAL CHEMISTRY LETTERS
Volume 12, Issue 21, Pages 5123-5131

Publisher

AMER CHEMICAL SOC
DOI: 10.1021/acs.jpclett.1c01206

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Funding

  1. European Research Council grant FORWARD [771688]
  2. European Research Council (ERC) [771688] Funding Source: European Research Council (ERC)

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This study brings fresh insights into the ensemble properties of PbS colloidal quantum dots by conducting experiments to investigate the radiative recombination of thermalized photocarriers. A phenomenological model based on the Kirchhoff law is proposed to identify the nature of the thermalized photocarriers and extract their temperatures. Two thermalization regimes are observed: one involving photocarriers distributed over a wide energy range and the other solely involving fundamental excitons.
We bring fresh insight into the ensemble properties of PbS colloidal quantum dots with a critical review of the literature on semiconductors followed by systematic comparisons between steady-state photocurrent and photoluminescence measurements. Our experiments, performed with sufficiently low powers to neglect nonlinear effects, indicate that the photoluminescence spectra have no other noticeable contribution beside the radiative recombination of thermalized photocarriers (i.e., photocarriers in thermodynamic quasi-equilibrium). A phenomenological model based on the local Kirchhoff law is proposed that makes it possible to identify the nature of the thermalized photocarriers and to extract their temperatures from the measurements. Two regimes are observed: For highly compact assemblies of PbS quantum dots stripped from organic ligands, the thermalization concerns photocarriers distributed over a wide energy range. With PbS quantum dots cross-linked with 1,2-ethanedithiol or longer organic ligand chains, the thermalization concerns solely the fundamental exciton and can quantitatively explain all the observations, including the precise Stokes shift between the absorbance and luminescence maxima.

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