Properties and the inclusion behavior of 6-O-alpha-D-galactosyl- and 6-O-alpha-D-mannosyl-cyclodextrins

The novel heterogeneous branched cyclodextrins (CDs), 6-O-alpha-D- galactosyl-alpha, -beta, and -gamma CDs (Gal-alpha, -beta, and -gamma CDs) and 6-O-alpha-D-mannosyl-alpha, -beta, and -gamma CDs (Man-alpha, -beta, and -gamma CDs) dissolved sufficiently in water and in 10-50% (v/v) methanol aqueous solutions, as did the homogeneous branched CDs, 6-O-alpha-D-glucosyl-alpha, -beta, and -gamma CDs (Glc-alpha, -beta, and -gamma CDs). The solubilities of heterogeneous branched CDs were higher than those of each parent non-branched CDs. The hemolytic activities of heterogeneous and homogeneous branched CDs were lower than those of each parent non-branched CDs and the hemolytic activity became weaker in the order of non-branched CD > Man-CD > Glc-CD > Gal-CD in each series of alpha, beta, and gamma CD. AL type solubility-phase diagrams were displayed in the formation of inclusion complexes of the guest compounds of small size (methyl benzoate, estriol, and dexamethasone) with Gal-, Man-, and Glc-CDs, and marked differences among the three kinds of branched CDs could not be detected. However, solubility-phase diagrams between these branched CDs and the insoluble guest compounds of large cyclic structure (cyclosporin A, tacrolimus, and amphotericin B) showed AP type, and the improvement of water solubilities of these guest compounds with three kinds of branched CDs was enhanced in the order of Man-CDs > Glc-CDs > Gal-CDs.     

Transfer of diclofenac sodium across excised guinea pig skin on high-frequency pulse iontophoresis. I. Equivalent circuit model

High frequency pulse iontophoresis of diclofenac sodium across excised guinea-pig skin was carried out in vitro. An equivalent circuit model was constructed to simulate the time courses of voltage drop across the donor solution and the skin. Parameter values obtained by the least-squares adaptation of the model to observed data were consistent with expectation and validated the proposed model.     

Unisized two-dimensional platinum clusters on silicon(111)-7x7 surface observed with scanning tunneling microscope

Uni-sized platinum clusters (size range of 5-40) on a silicon(111)-7 x 7 surface were prepared by depositing size-selected platinum cluster ions on the silicon surface at the collision energy of 1.5 eV per atom at room temperature. The surface thus prepared was observed by means of a scanning tunneling microscope (STM) at the temperature of 77 K under an ambient pressure less than 5 x 10(-9) Pa. The STM images observed at different cluster sizes revealed that (1) the clusters are flattened and stuck to the surface with a chemical-bond akin to platinum silicide, (2) every platinum atom occupies preferentially the most reactive sites distributed within a diameter of approximately 2 nm on the silicon surface at a cluster size up to 20, and above this size, the diameter of the cluster increases with the size, and (3) the sticking probability of an incoming cluster ion on the surface increases with the cluster size and reaches nearly unity at a size larger than 20.     

Analysis of toxic elements by MPGA

In order to improve the sensitivity for the quantification of trace elements, we propose the combination of prompt gamma-ray analysis (PGA) and a multiple gamma-ray detection method. A new Ge detector system for multiple prompt gamma-ray analysis (MPGA) was constructed at the neutron guide-hall of the JRR-3M reactor of the Japan Atomic Energy Agency (JAEA). The first demonstration of this system was given with a plastic sample containing traces of cadmium. The quantification limit of cadmium in a plastic sample was found to be about 0.1 ppm.     

Phase equilibrium in the system Ln-Mn-O: V. Ln=Yb and Dy at 1100°C

Phase equilibrium was established in the Yb-Mn-O and Dy-Mn-O systems at 1100°C by varying the oxygen partial pressure from −log (P_O2/atm)=0-13.00, allowing construction of phase diagrams at 1100°C for the systems Ln₂O₃-MnO-MnO₂. Under experimental conditions, Yb₂O₃, MnO, Mn₃O₄, and YbMnO₃ phases are found to be present in the Yb-Mn-O system, whereas Dy₂O₃, MnO, Mn₃O₄ DyMnO₃, and DyMn₂O₅ phases are present in the Dy-Mn-O system. Ln₂MnO₄, Mn₂O₃, and MnO₂ are not stable in either system. Small nonstoichiometric ranges are found in the LnMnO₃ phase, with the nonstoichiometry represented by the equations, N_O/N_YbMnO3=1.00×10⁻⁴(log P_O2)³+1.30×10⁻³(log P_O2)²+7.20×10⁻³(log P_O2)+5.00×10⁻⁵ and N_O/N_DyMnO3=1.00×10⁻⁴(log P_O2)³+1.80×10⁻³(log P_O2)²+9.30×10⁻³(log P_O2)+1.69×10⁻². Activities of the components in the solid solutions are calculated using these equations. LnMnO₃ may range Ln₂O₃-rich to Ln₂O₃-poor, while MnO is slightly nonstoichiometric to the oxygen-rich side. DyMn₂O₅ also seems to be nonstoichiometric. Lattice constants of LnMnO₃ under different oxygen partial pressures were determined, as well as lattice constants of DyMn₂O₅ quenched in air. The standard Gibbs energy changes of reactions appearing in the phase diagrams were calculated.     

A measurement on electromagnetic noise and change of surface inarcing electric contacts

The authors have observed the relationship between waveform of electromagnetic noise and change of surface for opening Ag-Pd electric contacts. In case of Ag-Pd electrodes, continuous noise is observed in the whole period of arc discharge in both current polarities. Fluctuations of are voltage and noise are large in the middle part of arc discharge duration. The noise decreases in the later half. The authors proposed a classification of noise waveforms and pattern of surface changes. As a result, patterns of noise waveform and changes of electrode surface at various circuit conditions are classified into three categories. In this paper, the authors showed the correlation between pattern of noise waveform and the change of electrode surface