The decay of the transient Photo-ElectroMotive-Force U(Photo-E.M.F.) of org
anic dye pigments can be described as a biexponential process, even if the
signals change the sign of U(t) within the decay. The dependencies of the f
our kinetic parameters U-1(0); U-2(0); k(1) and k(2) on wavelength and inte
nsity of the exciting laser flash or additional continuous illumination wer
e investigated using N,N'-Dimethylperylene-tetracarboxylic-bisimide (MePe)
and Copper(II)-phthalocyanine (CuPc) as pigments dispersed in polyvinyl but
yral (PVB) layers.
In agreement with the trap concept of MOTT the type of conductivity (n- or
p-type photoconduction) of MePe depends on the energy of the exciting light
. CuPc does not show such a change of the photoconduction.
More detailed information about the role of traps available for photogenera
ted charge carriers can be derived from time resolved Photo-E.M.F. experime
nts under additional continuous illumination of the sample by poly- and mon
ochromatic light. The results show, that charge carriers involved in Photo-
E.M.F. measurements will be infuenced mainly by shallow traps (DeltaE in th
e meV-range).
Occupation of traps by charge carriers generated under continuous illuminat
ion results in an increase of the decay rate for the faster process. This p
oints out, that its parameters U-1(0) and k(1) may be attributed to a parti
al Photo-E.M.F. generated near the surface of the pigment particles.