3 years ago

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

Mid-Gap States and Normal vs Inverted Bonding in Luminescent Cu+- and Ag+-Doped CdSe Nanocrystals
Daniel R. Gamelin, Stijn O. M. Hinterding, Rachel Fainblat, Xiaosong Li, Heidi D. Nelson, Sidney E. Creutz
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 (∼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 (∼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 display similar broad PL with large Stokes 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+ to Cu2+, in Ag+: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 Cu+ to Ag+. The spectroscopic similarities are explained by the fact that, in both materials, photogenerated holes are localized primarily within covalent [MSe4] dopant clusters (M = Ag+, Cu+). These findings reconcile the similar spectroscopies of Ag+- and Cu+-doped semiconductor NCs with the vastly different ionization potentials of their Ag+ and Cu+ dopants.

Publisher URL: http://dx.doi.org/10.1021/jacs.7b01924

DOI: 10.1021/jacs.7b01924

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