A. Vaes et al., TIME-RESOLVED PHOTOCURRENTS IN LANGMUIR-BLODGETT-FILMS OF SUBSTITUTEDHEXAALKOXYTRIPHENYLENE, Journal of applied physics, 84(1), 1998, pp. 339-349
By successive deposition of monolayers of the hexaalkoxytriphenylene d
erivative Te(OH)(2), organized multilayers with a thickness between 18
and 360 Angstrom can be obtained. Photoexcitation of the Langmuir-Blo
dgett films, deposited on interdigitating electrodes with a spacing of
100 mu m, by a laser pulse of 4 ns full width at half maximum at a wa
velength of 320 nm and with an energy between 5 and 200 mu J, induces
transient photocurrents. At large applied fields or upon increasing th
e energy of the laser pulse and at-reduced pressure, besides a transie
nt current pulse of which the features are determined by the bandwidth
of the experimental setup, a second current pulse grows in and shows
a maximum at 1.5 mu s after excitation. At low fields, charge generati
on occurs mainly in the bulk of the sample. In this field range, most
charge carriers disappear by trapping or recombination before they can
reach the opposite electrode, making it difficult to get information
about the transit time. In the high field range, the charge carriers a
re still due to light absorbed by the Te(OH)(2) layers. In this field
range, the pressure of air dr nitrogen strongly influences the feature
s of the second maximum. The observation of the second maximum above a
critical voltage and under optimal pressure conditions, suggests that
corona discharging is also an important process. According to this mo
del, the second maximum is related with the transit time of the charge
carriers which migrate perpendicular to the substrate. (C) 1998 Ameri
can Institute of Physics.