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Low intensity, continuous wave photodoping of ZnO quantum dots - photon energy and particle size effects.

作者信息

Aguirre Matías E, Municoy S, Grela M A, Colussi A J

机构信息

Instituto de Investigaciones Físicas de Mar del Plata (IFIMAR)-Departamento de Química, Facultad de Ciencias Exactas y Naturales, Universidad Nacional de Mar del Plata-CONICET, Funes 3350, (7600) Mar del Plata, Prov. de Buenos Aires, Argentina.

Departamento de Micro y Nanotecnología, GAIANN - Centro Atómico Constituyentes, Comisión Nacional de Energía Atómica, Av. Gral. Paz 1499 - (1650), San Martín, Prov. de Buenos Aires, Argentina.

出版信息

Phys Chem Chem Phys. 2017 Feb 8;19(6):4494-4499. doi: 10.1039/c6cp06829d.

DOI:10.1039/c6cp06829d
PMID:28120971
Abstract

The unique properties of semiconductor quantum dots (QDs) have found application in the conversion of solar to chemical energy. How the relative rates of the redox processes that control QD photon efficiencies depend on the particle radius (r) and photon energy (E), however, is not fully understood. Here, we address these issues and report the quantum yields (Φs) of interfacial charge transfer and electron doping in ZnO QDs capped with ethylene glycol (EG) as a function of r and E in the presence and absence of methyl viologen (MV) as an electron acceptor, respectively. We found that Φs for the oxidation of EG are independent of E and photon fluence (φ), but markedly increase with r. The independence of Φs on φ ensures that QDs are never populated by more than one electron-hole pair, thereby excluding Auger-type terminations. We show that these findings are consistent with the operation of an interfacial redox process that involves thermalized carriers in the Marcus inverted region. In the absence of MV, QDs accumulate electrons up to limiting volumetric densities ρ that depend sigmoidally on excess photon energy E* = E - E(r), where E(r) is the r-dependent bandgap energy. The maximum electron densities: ρ ∼ 4 × 10 cm, are reached at E* > 0.5 eV, independent of the particle radius.

摘要

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