The main target organ of the mycotoxin ochratoxin A (OTA) in mammals is the kidney but OTA has also been shown to be hepatotoxic in rats and to induce tumors in mouse liver. Even at very low concentrations, OTA causes perturbations of cellular signaling pathways as well as enhanced apoptosis. OTA has been extensively studied in kidney cell systems. Since this substance also affects liver health, we focused our work on apoptosis-related events induced by OTA in primary rat hepatocytes. We performed pathway-specific polymerase chain reaction arrays to assess the expression of genes involved in apoptosis. Treatment with 1 microM OTA for 24 h caused marked changes in apoptosis-related gene expression. Genes as apaf1, bad, caspase 7, polb (DNA polymerase beta, performs base excision repair), and p53, which are marker genes for DNA damage, were upregulated. FAS and faslg were also markedly induced by treatment with OTA. Treatment of hepatocytes with OTA led to a concentration-dependent inhibition of protein biosynthesis. Apoptosis-inducing factor was released from mitochondria following OTA treatment; the mycotoxin induced the activity of caspases 8, 9, and 3/7 and caused chromatin condensation and fragmentation. Caspase inhibition led to a significant but not complete reduction of OTA-induced apoptosis. Our data suggest that not only OTA leads to p53-dependent apoptosis in rat hepatocytes but it also hints to other mechanisms, independent of caspase activation or protein biosynthesis, being involved.

The valence state of Yb in YbC(2) was analyzed using high-energy-resolution fluorescence detection (HERFD) X-ray absorption near-edge structure (XANES) spectroscopy and time-of-flight neutron powder diffraction to clarify a controversy in the literature. The unit cell volume of YbC(2) suggests a mixed Yb valence, which was formerly determined to be 2.8 by magnetization measurements and paramagnetic neutron scattering techniques. However, the nature of the intermediate valence was not clearly established. Both homogeneous and heterogeneous mixed valences were assumed in different publications. The temperature-dependent behavior of the valence state was only predicted, albeit not explicitly studied. In this work, the valence state of Yb in YbC(2) is, therefore, investigated thoroughly by HERFD-XANES spectroscopy at low and high temperatures. Our measurements result in an average Yb valence of 2.81 that is temperature-independent from 15 to 1123 K. These findings are confirmed by neutron powder diffraction experiments, which reveal a constant C-C distance of 128.7(9) pm in a temperature range from 5 to 100 K. A significant temperature dependence of the Yb valence state in YbC(2) can, therefore, be excluded by our experimental results.

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Pure EuC(2), free of EuO impurities, was obtained by the reaction of elemental europium with graphite at 1673 K. By means of synchrotron powder diffraction experiments, the structural behavior was investigated in the temperature range from 10 to 1073 K. In contrast to former results, EuC(2) crystallizes in the ThC(2) type structure (C2/c, Z = 4) at room temperature. A tetragonal modification (I4/mmm, Z = 2) is only observed in a very small temperature range just below the transition to a cubic high-temperature modification (Fm3m, Z = 4) at 648 K. DTA/TG investigations confirm these results. According to Raman spectroscopy, EuC(2) contains C(2)(2-) ions (nu(C[triple bond]C) = 1837 cm(-1)). The divalent character of Eu is confirmed by the results of magnetic susceptibility measurements and (151)Eu Mossbauer spectroscopy. In these measurements a transition to a ferromagnetic state with T(C) = 15 K is observed, which is in reasonable agreement with literature data. Above T(C) EuC(2) is a semiconductor according to measurements of the electric resistivity vs temperature, again in contrast to former results. Around T(C) a sharp maximum of the electric resistivity vs temperature curve was observed, which collapses on applying external magnetic fields. The observed CMR effect (colossal magnetoresistance) is much stronger than that reported for other EuC(2) samples in the literature. These investigations explicitly show the influence of sample purity on the physical and even structural properties of EuC(2).

Table 1 contains several typos and inconsistencies. A revised table is given below. Revised CIFs for each structure are deposited at FIZ Karlsruhe and are given as Supporting Information.We are thankful to Michael H€ ulsen for indicating the inconsistencies in Table 1.