Simple template-based method to produce bradbury-nielsen gates

A Bradbury-Nielsen gate (BNG) consists of two interleaved and electrically isolated sets of wires and can transmit or deflect charged particles by applying a varying voltage difference across the two wire sets. We present a simple template-based method to fabricate BNGs with wire spacings as small as 50 microm with minimal use of a microscope. The small wire spacing allows modulation rates at tens of megahertz. Using this method, we have fabricated four BNGs with wire spacings of 500, 200, 100, and 50 microm using 10 microm gold-coated tungsten wires. The performance of the four BNGs is characterized using an imaging detector and compared with theoretical predictions.     

Catalytic activity of H3PMo12?XWXO40 and H6P2MO18?XWXO62 heteropolyacid (HPA) catalysis in the direct preparation of dichloropropanol (DCP) from glycerol

H₃PMo_12−XWXO₄₀ (X=0−12) and H₆P₂Mo_18−XWXO₆₂ (X=0−18) heteropolyacid catalysts were applied to the direct preparation of dichloropropanol from glycerol. Acid properties of the catalysts were determined by NH₃-TPD measurements. The catalytic performance increased with increasing acid strength of the catalyst. Among the catalysts tested, the H₃PW₁₂O₄₀ catalyst of highest acid strength showed the best catalytic performance.     

Conformational study of jet-cooled L-phenylglycine

We investigated the conformational structures of L-phenylglycine in the gas phase by photoionization and double resonance spectroscopy techniques as well as high-level ab initio calculations. The UV-UV and IR-UV double resonance spectroscopy suggested that there exists only one conformer that has a free OH band for the carboxyl group. Rotational contour analysis combined with ab initio calculation indicated that the conformer we detected by resonant two-photon ionization was not one of those found by Sanz et al. in their microwave spectroscopic study [Chem. Eur. J. 12, 2564 (2006)]. Different methods of vaporization along with different expansion and cooling conditions and different detection methods are believed to be the culprit for such intriguing discrepancy. The identical hydrogen bonding structure of our phenylglycine conformer with the most abundant conformer of glycine found in helium droplets and their nearly identical OH frequencies suggest that the skeletal structure of glycine is not significantly altered by phenyl substitution.     

Conformationally specific vacuum ultraviolet mass-analyzed threshold ionization spectroscopy of alkanethiols: structure and ionization of conformational isomers of ethanethiol, isopropanethiol, 1-propanethiol, tert-butanethiol, and 1-butanethiol

Conformational isomers of alkanethiols are isolated in the molecular beam, and the conformer-specific ionization dynamics have been investigated using vacuum ultraviolet mass-analyzed threshold ionization (MATI) spectroscopy. Only a single conformer of ethanethiol is observed to give the adiabatic ionization potential (IP) of 9.2922 +/- 0.0007 eV for the gauche conformer. For isopropanethiol, IP is found to be 9.1426 +/- 0.0006 for the trans conformer and 9.1559 +/- 0.0006 eV for the gauche conformer. Only two major conformational isomers are identified for 1-propanethiol, giving an IP of 9.1952 +/- 0.0006 for the trans-gauche conformer and 9.2008 +/- 0.0006 eV for the gauche-gauche conformer. The tert-butanethiol, as expected, has a single conformer with an IP of 9.0294 +/- 0.0006 eV. For 1-butanethiol, there are a number of conformers, and the assignment of the MATI bands to each conformer turns out to be nontrivial. The spectral simulation using the Franck-Condon analysis based on the density functional theory (DFT) calculations has been used for the identification of each conformational isomer in the MATI spectrum. Each conformer undergoes its unique structural change upon ionization, as revealed in the vibration resolved MATI spectrum, providing the powerful method for the spectral identification of a specific conformational isomer. The conformer specificity in the ionization-driven structural change reflects the role of the electron of the highest occupied molecular orbital (HOMO) in the conformational preference.     

Crystalline-amorphous interaction in relation to the phase diagrams of binary polymer blends containing a crystalline constituent

The present article describes an equilibrium theory for determining binary phase diagrams of various crystalline-amorphous polymer blends by taking into account the contributions from both liquid-liquid phase separation between the constituents and solid-liquid phase transition of the crystalline component. An analytical expression for determining a crystal-amorphous interaction parameter is deduced based on the solid-liquid transition, involving the solidus and liquidus lines in conjunction with the coexistence curve of an upper critical solution temperature type. Of particular importance is that the crystalline-amorphous interaction parameter can be determined directly from the melting point depression data. The present analysis is therefore different from the conventional Flory-Huggins interaction parameter, which is associated with the liquid-liquid phase separation. The validity of the present theory is tested with the experimental phase diagrams of blends of poly(ethylene oxide)/diacrylate and poly(vinyl alcohol)/cellulose.     

Structure of Pyridazine in the S1 State: Experiment and Theory

The molecular structure of pyridazine in the first electronically excited state (S₁) is deduced from the combined use of resonance‐enhanced two‐photon ionization and mass‐analyzed threshold ionization spectroscopic methods. The equation‐of‐motion coupled‐cluster single and double (EOM–CCSD) calculation gives the distorted planar geometry for the most stable structure of the S₁ pyridazine. The symmetry constraint of C_2v is relaxed to that of C_s, and consequently many in‐plane vibrational modes are found to be optically active in both S₁–S₀ and D₀–S₁ excitation spectra, being appropriately assigned from the comparison of their frequencies with ab initio values. This indicates that the S₁–S₀ excitation is partially localized, and provides an alternative explanation for the long‐standing spectroscopic puzzle in S₁ pyridazine.     

Regulation of cell growth by fatty acid-CoA ligase 4 in human hepatocellular carcinoma cells

Fatty acid-CoA ligase 4 (FACL4) is a central enzyme controlling the unesterified free arachidonic acid (AA) level in cells and the free AA is known to induce apoptosis. We have recently reported that expression of FACL4 is upregulated in about 40% of human hepatocellular carcinoma (HCC) and 50% of HCC cell lines, suggesting that FACL4 may be involved in liver carcinogenesis. In this study, we investigated whether HCC cell growth is regulated by FACL4. Immunoblot analysis showed that SNU 398 cells express very low or no detectable level of FACL4. We, therefore, transfected the SNU 398 cells with FACL4 expression vector, and clones expressing FACL4 were pooled and analyzed. We found that forced expression of FACL4 in SNU 398 promotes the growth of cells. In addition, we observed that triacsin C, a FACL4 inhibitor, inhibits the growth of Hep 3B cell line which expresses high level of endogenous FACL4. We also found that the triacsin C-mediated growth inhibition in Hep 3B cells results from the induction of apoptosis with evidence of Bcl-2 reduction. Altogether, our data show that FACL4 affects HCC cell growth and suggest that modulation of FACL4 expression/activity is an approach for treatment of HCC.     

Photophysical properties and energy transfer pathway of Er(III) complexes with Pt-porphyrin and terpyridine ligands

The photophysical properties of Er(III) complexes coordinated with platinum[5,10,15-triphenyl-20-(4-carboxyphenyl)-porphyrin] (PtP) and terpyridine (tpy) ligands in organic solution were investigated. The Er(III) complex emitted sensitized near-IR (NIR) luminescence when the PtP ligands were excited under deoxygenated conditions. The quantum yield (PhiLn) of the sensitized luminescence was 0.015%, as evaluated from luminescence lifetime. The photophysical studies and theoretical calculations suggest that the F?rster resonance mechanism is very suitable for the energy transfer from PtP to the Er(III) ion and occurred through the first triplet excited state of PtP. The 12.3% energy transfer from the triplet state to the 4F9/2 and 4I9/2 states of Er(III) occurred with a rate distribution of 3.36x10(5) and 6.67x10(4) s(-1), respectively. In addition, the observed triplet quantum yield of the PtP ligand in [Ln(PtP)3(tpy)] proved that the energy transfer from the singlet excited state of the PtP ligand to the Er(III) ion did not take place.