Photovoltage (PV) transients are studied in C60–Pb and C60–Au thin films. The morphology of the C60 layers is characterized by x-ray diffraction and atomic force microscopy, which evidence the formation of a nanocrystalline C60 layer on polycrystalline Pb and Au underlayers. In contrast to Au substrate, Pb crystallites with a (111) texture are predominantly formed. The signs of the PV signals developed at the C60–Pb and C60–Au interfaces are found to be opposite due to very different workfunction values of the two metals. The evolution of the PV rise and decay curves with increasing light illumination intensity is completely different at the C60–Pb and C60–Au interfaces. The rise for the C60–Pb interface speeds up considerably with the increase in intensity, which is markedly different from the behavior at C60–Au, which exhibits nearly unchanged curve shapes. The PV decay time for C60–Au is also only weakly affected by varying light intensity. In contrast, increasing the illumination intensity causes the decay curves for C60–Pb to become multiexponential profiles, developing fast initial decays. The results are discussed in terms of different charge redistribution properties of C60 molecules adsorbed on Pb(111) and Au interfaces. The observed transformation of the PV decay curves is explained by the presence of interface states and a subsequent interplay of the charge redistribution properties of C60 molecules adsorbed on Pb(111). The results can be applied to sandwich structures containing organic-metal interfaces to account correctly for the interfacial charge transfer dynamics.

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The measurements of the real part of the dielectric constant and X‐ray diffraction studies of different polytypes of TlInS2 crystals are presented in the temperature range T = 160–250 K. Substantial influence polytypism on the occurrence of a polarized state in TlInS2 crystals has been revealed. It is shown that phase transition in 2C‐polytype, unlike C‐polytype, is not accompanied by a quadrupling of elementary cell along C axes, it is characterized by the other order parameter and occurs at higher temperatures.(© 2009 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)