This paper describes the use of visible, near-infrared, and mid-infrared steadystate optical spectroscopy to study the geometries in which tetracyanoquinodimethane (TCNQ) adsorbs to the surfaces of highly cadmium enriched and near-stoichiometric CdSe quantum dots (QDs) in the formation of QD-TCNQ charge transfer (CT) complexes. Several TCNQ molecules are spontaneously reduced by chalcogenides on the surface of each CdSe QD. The degree of CT depends on the geometry with which the TCNQ adsorbs and the degree of distortion of TCNQ's geometry upon adsorption. Comparison of the electronic and vibrational spectra of CdSe QD-TCNQ complexes with those of CT complexes of TCNQ with molecular reductants (including molecular chalcogenides) and computer simulations of the geometries and vibrational spectra of the TCNQ-chalcogenide CT complexes show that (i) the Cd-enriched CdSe QDs reduce a factor of 7.4 more TCNQ molecules per QD than nearly stoichiometric CdSe QDs because surface selenides are more accessible in the Cdenriched QDs than in the near-stoichiometric QDs and (ii) TCNQ interacts with surface selenides through several adsorption modes that result in different amounts of charge transfer and different degrees of geometric distortion of TCNQ. This study provides a framework for determining the range of adsorption geometries of small molecules on QD surfaces, and for optimizing QD surfaces to adsorb molecules in configurations with maximal electronic coupling between the QD and the adsorbate.
■ INTRODUCTIONThis paper describes the use of visible, near-infrared, and midinfrared steady-state optical spectroscopy to determine the set of geometries in which tetracyanoquinodimethane (TCNQ) adsorbs to the surfaces of CdSe quantum dots (QDs) in the formation of QD-TCNQ charge transfer (CT) complexes, and the dependence of these geometries on the surface chemistry of the QDs. Metal-chalcogenide QDs have high absorption cross sections, for instance, factors of ten to 100 greater than that of the metal-to-ligand charge transfer absorption band of ruthenium(II)tris(bipyridine) (Ru(bpy) 3 2+ ), 1 for bandgapresonant excitations across the long-UV, visible, and nearinfrared regions of the solar spectrum. 2 This optical bandgap can be tuned with both the material and size of the QD. 2 They also have the ability to accumulate multiple simultaneous excitons or charge carriers within a single nanoparticle. These properties make QDs potentially important as chromophores and redox centers within photovoltaic and photocatalytic active materials. For both types of devices, efficient extraction of charge carriers from the QDs is critical to the performance of the device. We have shown previously that, in order for ultrafast (tens of picoseconds or faster) charge transfer between a QD and a molecule to occur, the molecule must permeate the ligand shell of the QD and adsorb, at least transiently, to its inorganic surface. 3,4 It is therefore important to know what types of surface chemistries promote adsorption of potential molecular redox p...