4.8 Article

Mid-Gap States and Normal vs Inverted Bonding in Luminescent Cu+- and Ag+-Doped CdSe Nanocrystals

期刊

JOURNAL OF THE AMERICAN CHEMICAL SOCIETY
卷 139, 期 18, 页码 6411-6421

出版社

AMER CHEMICAL SOC
DOI: 10.1021/jacs.7b01924

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资金

  1. National Science Foundation [DGE-1256082, CHE-1565520, DMR-1505901]
  2. Stichting Fundatie van de Vrijvrouwe van Renswoude to 's-Gravenhage
  3. Stichting dr. Hendrik Muller's Vaderlandsch Fonds
  4. German Academic Exchange Service (DAAD)
  5. German Federal Ministry of Education and Research (BMBF)
  6. People Programme (Marie Curie Actions) of the European Union's Seventh Framework Programme (FP7) [605728]
  7. UW Student Technology Fee
  8. Division Of Materials Research
  9. Direct For Mathematical & Physical Scien [1505901] Funding Source: National Science Foundation

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Mid-gap luminescence in copper (Cu+)-doped semiconductor nanocrystals (NCs) involves recombination of delocalized conduction-band electrons with copper-localized holes. Silver (Ag+)-doped semiconductor NCs show similar mid gap luminescence at slightly (similar to 0.3 eV) higher energy, suggesting a similar luminescence mechanism, but this suggestion appears inconsistent with the large difference between Ag+ and Cu+ ionization energies (similar to 1.5 eV), which should make hole trapping by Ag+ highly unfavorable. Here, Ag+-doped CdSe NCs (Ag+ :CdSe) are studied using time-resolved variable-temperature photoluminescence (PL) spectroscopy, magnetic circularly polarized luminescence (MCPL) spectroscopy, and time dependent density functional theory (TD-DFT) to address this apparent paradox. In addition to confirming that Ag+:CdSe and Cu+:CdSe NCs shifts, we demonstrate that both also show very similar temperature-dependent PL lifetimes and magneto-luminescence. Electronic-structure calculations further predict that both dopants generate similar localized mid-gap states. Despite these strong similarities, we conclude that these materials possess significantly different electronic structures. Specifically, whereas photogenerated holes in Cu+:CdSe NCs localize primarily in Cu(3d) orbitals, formally oxidizing Cu-i- to Cu', in Agt:CdSe NCs they localize primarily in 4p orbitals of the four neighboring Se2- ligands, and Ag is not oxidized. This difference reflects a shift from normal to inverted bonding going from Cut to Agt. The spectroscopic similarities are explained by the fact that, in both materials, photogenerated holes are localized primarily within covalent [MSe4] dopant clusters (M = Agt, Cut). These findings reconcile the similar spectroscopies of Agt and Cut-doped semiconductor NCs with the vastly different ionization potentials of their Ag+ and Cu+ dopants.

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