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Hole transport in porphyrin thin films
Author(s) -
Tom J. Savenije,
Albert Goossens
Publication year - 2001
Publication title -
physical review. b, condensed matter
Language(s) - English
Resource type - Journals
eISSN - 1095-3795
pISSN - 0163-1829
DOI - 10.1103/physrevb.64.115323
Subject(s) - photocurrent , porphyrin , physics , materials science , amorphous solid , acceptor , heterojunction , thin film , analytical chemistry (journal) , atomic physics , condensed matter physics , crystallography , nanotechnology , optics , photochemistry , chemistry , chromatography
Hole transport in p-type organic semiconductors is a key issue in the development of organic electronic devices. Here the diffusion of holes in porphyrin thin films is investigated. Smooth anatase TiO2 films are coated with an amorphous thin film of zinc-tetra~4-carboxyphenyl! porphyrin ~ZnTCPP! molecules acting as sensitizer. Optical excitation of the porphyrin stimulates the injection of electrons into the conduction band of TiO2. The remaining holes migrate towards the back electrode where they are collected. Current-voltage and capacitance-voltage analysis reveal that the TiO 2 / ZnTCPP system can be regarded as an n- p heterojunction, with a donor density of ND52.0310 16 cm 23 for TiO2 and an acceptor density NA54.0310 17 cm 23 for ZnTCPP films. The acceptor density in porphyrin films increases to 1.3 310 18 cm 23 upon irradiation with 100-mW cm 22 white light. Intensity-modulated photocurrent spectroscopy, in which ac-modulated irradiation is applied, is used to measure the transit times of the photogenerated holes through the films. A reverse voltage bias hardly affects the transit time, whereas a small forward bias yields a decrease of the transit time by two orders of magnitude. Application of background irradiation also reduces the transit time considerably. These observations are explained by the presence of energy fluctuation of the highest-occupied molecular orbital level in the porphyrin films due to a dispersed conformational state of the molecules in the amorphous films. This leads to energetically distributed hole traps. Under short circuit and reverse bias, photogenerated holes reside most of the time in deep traps and their diffusivity is only 7 310 211 cm 2 s 21 . Deep traps are filled by application of a forward bias and by optical irradiation leading to reduction of the transit time and a concomitant increase of the diffusivity up to 2 310 27 cm 2 s 21 .

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