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In this article several aspects concerning the induction of magnetic ordering in graphite via proton bombardment using nuclear nanoprobes are addressed such as proton range and lateral straggling, defect densities, heat load, and simultaneous impurity analysis via particle induced X-ray emission.

The tensile properties and microstructures of AA6061/SiCp composites fabricated by the pressureless infiltration method under a nitrogen atmosphere were examined. Since the spontaneous infiltration of molten AA6061 into the powder bed containing SiCp occurred at 800 °C for 1 hour under a nitrogen atmosphere, it was possible to fabricate composites reinforced with SiCp. Reaction product (Al 4 C 3 ) was formed at the interface between SiCp and Al alloy matrix. In addition, the amount and size of the Al 4 C 3 is increased significantly by increasing the infiltration temperature. The reaction product (AlN) was formed as a result of the in situ reaction in both the control alloy and the composite. A significant strengthening even in the control alloy occurred due to the formation of in situ AIN particle even without an addition of SiCp. While a further strengthening of the composite was produced by the reinforced SiCp, strain to failure of the composite fabricated at 800 °C showed the lowest value (1.3%) in the T6 condition due to the formation of the severe reaction product (Al 4 C 3 ). The grain size of the control alloy significantly decreased to about 20 μm compared to 50 μm for the commercial alloy. In addition, the grain size in the composite reinforced with SiCp further decreased to about 8.0 μm. This grain refinement contributed to strengthening of the control alloy and composite.

A recurring problem with cancer therapies is the development of drug resistance. While investigating the protein profile of cells resistant to a novel antimitotic compound (A204197), we discovered an increase in annexin IV expression. When we examined the annexin IV protein expression level in a paclitaxel-resistant cell line (H460/T800), we found that annexin IV was also overexpressed. Interestingly a closely related protein, annexin II, was not overexpressed in H460/T800 cells. Immunostaining with either annexin II or IV antibody revealed that annexin IV was primarily located in the nucleus of paclitaxel-resistant H460/T800 cells. Short-term treatment of H460 cells with 10 nMpaclitaxel for up to 4 days resulted in induction of annexin IV, but not annexin II expression. In addition, there was an increase in annexin IV staining in the nucleus starting at day 1. Furthermore, cells pretreated with 10 nMpaclitaxel for 4 days resulted in cells becoming ~fivefold more resistant to paclitaxel. Transfection of annexin IV cDNA into 293T cells revealed that there was a threefold increase in paclitaxel resistance. Thus our results indicate that annexin IV plays a role in paclitaxel resistance in this cell line and it is among one of the earliest proteins that is induced in cells in response to cytotoxic stress such as antimitotic drug treatment. © 2000 Cancer Research Campaign

To clarify the roles of specific isoforms of PKC in regulating growth and cell cycle progression of the HC11 mammary epithelial cell line, we investigated the effects of activating endogenous PKC isoforms with the phorbol ester tumor promoter TPA, and also the effects of TPA on genetically engineered cells containing increased levels of individual PKC isoforms. We found that TPA treatment of HC11 cells induced a transient cell cycle arrest in G0/G1. Western blot analyses of the TPA treated cells provided evidence that the endogenous PKC alpha present in these cells mediated these effects. Indeed, derivatives of the HC11 cell line that inducibly overexpress an exogenous PKC alpha or ectopic PKC beta 1 exhibited more marked growth inhibition by TPA than control cells. Immunohistochemical staining of cells following treatment with TPA revealed selective translocation of PKC alpha into the nucleus, whereas PKC beta 1 remained in the cytoplasm. The transient arrest of HC11 cells following treatment with TPA was associated with marked induction of both p21cip1 mRNA and protein. This induction was exaggerated in the derivatives that overexpressed either PKC alpha or PKC beta 1. Therefore, in mouse mammary epithelial cells activation of the endogenous PKC alpha can transiently arrest cells in G0/G1 which may be due, at least in part, to induction of the transcription of p21cip1.

It is now apparent that apoptosis is closely linked to the control of cell cycle progression. During the G1 to S progression, cyclin D1, p53, and the cyclin dependent kinase inhibitors p21WAF1 and p27kip1 can play roles in induction of apoptosis. During the G2 and M phases, premature activation of Cdk1 can cause cells to enter mitotic catastrophe, which results in apoptosis. In this review we focus on factors acting during G1 and S, particularly cyclin D1, and their effects on cell growth, senescence and apoptosis. We emphasize that cyclin D1 can have diverse effects on cells depending on its level of expression, the specific cell type, the cell context and other factors. Possible mechanisms by which cyclin D1 exerts these diverse effects, via cyclin dependent kinase-dependent and -independent pathways, are discussed.

Magnetic force microscopy (MFM) can be used to image current distributions in current leads of sub-micron dimensions. Here we present a systematic study about the spatial and force resolution of such currents. In the case of force resolution, we studied the least measurable magnetic force of MFM for different sample currents. The analysis of images from parallel Al conducting plates are combined with those from force-distance curves and finite element calculations. Several interacting regimes between the magnetic tip and the currents are found and interpreted. It is shown that model calculations are necessary even for qualitative image interpretation. Then spatial resolution in the range of 100nm can well be obtained and quantitative studies of current distribution on widths of 10nm resolution are possible in special cases. The approach is demonstrated in imaging the current distribution in superconducting Bi2Sr2CaCu2Ox single crystals.