Study of the kinetics of free volume in Zr45.0Cu39.3Al7.0Ag8.7 bulk metallic glasses during isothermal relaxation by enthalpy relaxation experiments

Enthalpy relaxation experiments were conducted to study the kinetics of free volume in Zr_45.0Cu_39.3Al_7.0Ag_8.7 bulk metallic glasses (BMGs) during isothermal relaxation using differential scanning calorimetry (DSC) at the temperature within the range from 648 to 684 K. Stretched exponential relaxation functions and the ?esták–Berggren SB (m, n) model were employed to analyze the kinetics of free volume. It is found that the relaxation time decreases from 2643.5 to 242.8 s while the Kohlrausch exponents increase from 0.717 to 0.892 in the investigated temperature range. The activation energy fluctuates slightly in the course of the relaxation process and its mean value is determined to be 239.7 kJ/mol. By fitting the first derivative of the conversion degree as a function of annealing time using the ?esták–Berggren SB (m, n) model, it is found that the values of m at all annealing temperatures are very small and can be approximated as zero. The values of the pre-exponential factors Z and the kinetic parameter n are found to be slightly varying with the annealing temperature, indicating the complexity of the kinetics of the isothermal relaxation. Finally, an approximate rate equation describing the kinetics of free volume during isothermal relaxation is proposed.     

Genotyping fetal paternally inherited SNPs by MALDI-TOF MS using cell-free fetal DNA in maternal plasma: influence of size fractionation

The determination of fetal point mutations from fetal cell-free DNA (cf-DNA) in maternal plasma is technically challenging due to the preponderance of maternal sequences. It has recently been shown that fetal cf-DNA sequences are smaller than maternal ones and that the selection of small cf-DNA fragments by size fractionation by agarose gel electrophoresis leads to the enrichment of fetal cf-DNA sequences, thereby permitting the detection of otherwise masked fetal point mutations. In a separate development, the use of MALDI-TOF MS has also been shown to facilitate the detection of fetal point mutations from cf-DNA in maternal plasma. In this study, a combination of these approaches was examined. cf-DNA was extracted from 18 maternal plasma samples, 10 taken at term and 8 obtained early in the second trimester. A total of 41 SNP loci were examined in size-fractionated and total cf-DNA using either a conventional homogeneous MassEXTEND (hME) assay or a nucleotide-specific single allele base extension reaction (SABER) assay. The analysis of total cf-DNA indicated that size fractionation considerably enhanced the sensitivity of the standard hME assay, especially for samples taken early in pregnancy. Size fractionation also rendered the signals obtained by the SABER assay more precise.     

Cathodic electrodeposition of mixed molybdenum tungsten oxides from peroxo-polymolybdotungstate solutions

Mixed molybdenum tungsten trioxide films of varying stoichiometry (MoxW1 - xO3, 0 < x < 1) were prepared by cathodic electrodeposition on indium tin oxide (ITO)-coated glass substrates from aqueous peroxo-polymolybdotungstate solutions. Electrochemical quartz crystal microbalance (EQCM), cyclic voltammetry, and chronocoulometry were used to gain insight into the electrodeposition mechanism. The compositional and structural properties were characterized for MoxW1 - xO3 films deposited at intermediate potentials (-0.35 V vs Ag/AgCl) and sintered at 250 degrees C using energy-dispersive spectroscopy, X-ray diffraction, and Raman spectroscopy. These studies reveal that films consist of homogeneously mixed MoxW1 - xO3, with an enriched Mo content ranging in composition from 0.4 < x < 0.7 depending upon the mol % Mo present in the deposition solution. Chronoamperometry and spectroelectrochemical measurements were conducted to estimate lithium ion diffusion coefficients and coloration efficiencies for the mixed metal oxide films in 1 M LiClO4/propylene carbonate. The subtle interplay between structural and compositional properties due to the uniform mixing of Mo and W oxide components shows that electrochromic and lithium ion transport properties are moderately enhanced relative to those of single-component WO3 and MoO3 and demonstrate improved structural stability over pure MoO3 polymorphs during electrochemical cycling.     

Site-specific hydrogen-bonding interaction between N-acetylproline amide and protic solvent molecules: comparisons of IR and VCD measurements with MD simulations

The effects of solute-solvent interactions on solution structures of small peptides have been paid a great deal of attention. To study the effect of hydrogen-bonding interactions on peptide solution structures, we measured the amide I IR and VCD spectra of N-acetylproline amide (AP) in various protic solvents, i.e., D2O, MeOD, EtOD, and PrOD, and directly compared them with theoretically simulated ones. The numbers of protic solvent molecules hydrogen-bonded to the two peptide bonds in the AP were quantitatively determined by carrying out the molecular dynamics (MD) simulations and then compared with the spectral analyses of the experimentally measured amide I bands. The two peptides in the AP have different propensities of forming H-bonds with protic solvent molecules, and the H-bond population distribution is found to be strongly site-specific and solvent-dependent. However, it is found that adoption of the polyproline II (PII) conformation by AP in protic solvents does not strongly depend on the hydrogen bond network-forming ability of protic solvents nor on the solvent polarity. We present a brief discussion on the validity as well as limitation of the currently available force field parameters used for the present MD simulation study.     

Structure of N-acetylproline amide in liquid water: experimentally measured and numerically simulated infrared and vibrational circular dichroism spectra

A few experimental and theoretical studies on the molecular structure of N-acetylproline amide (AP) in D2O solution have been reported recently. However, there is no consensus of the precise structure of AP in D2O because spectroscopically determined structures and a theoretically simulated one have been found to be different from one another. To determine its aqueous solution structure, IR and vibrational circular dichroism spectra of both L- and D-form AP solutions were measured. Molecular dynamics simulations with two different force fields and density functional theory calculations for the trans and cis rotamers of AP were performed to numerically simulate those spectra. Comparisons between experimentally measured and computationally simulated spectra directly suggest that the AP in water adopts a polyproline II-like conformation and that the force field parameter ff03 in the AMBER 8 suite of programs is more realistic and reliable in predicting molecular structure of AP in water than the ff99 in AMBER 7.     

Atomic structures of benzene and pyridine on Si(5 5 12)-2 x 1

The adsorption structures of benzene and pyridine on Si(5 5 12)-2 x 1 were studied at 80 K by using a low-temperature scanning tunneling microscope and density functional theory calculations. These structures are different from those observed on low-index Si surfaces: benzene molecules exclusively bind to two adatoms, that is, with di-sigma bonds between carbon atoms and silicon adatoms, leading to the loss of benzene aromaticity; in contrast, pyridine molecules interact with adatom(s) through either Si-N dative bonding or di-sigma bonds. Dative bonding configurations with pyridine aromaticity are the dominant adsorption features and are more stable than di-sigma bonding configurations. Thus the dative bonding of nitrogen-containing heteroaromatic molecules provides a strategy for the controlled attachment of aromatic molecules to high-index surfaces.     

A dinuclear triple-stranded helicate with a bis(benzene-o-dithiolato) ligand

The bis(benzene-o-dithiol) ligand H4-1 reacts with Ti4+ in a self-assembly reaction to give the dinuclear triple-stranded helicate [Ti2(1)3]4- which is the first helicate build exclusively from benzene-o-dithiolato donor groups.     

Synthesis,Characterization, and Properties of Tetraphenylethylene-Based Tetrakis-NHC Ligands and Their Metal Complexes

The development of highly emissive dinuclear Ag^I or Au^I complexes [M₂L](PF₆)₂ (L= 2 a , 2 b ; M=Ag, Au) derived from tetraphenylethylene (TPE)-based tetrabenzimidazolin-2-ylidene ligands is reported. The new complexes exhibit a remarkable fluorescence enhancement compared to their parent benzimidazolium salts. The quantum yield (Φ_F) value for salt H₄- 2 a (PF₆)₄ in dilute solution (c=10⁻⁵ m ) was found to be less than 1 %, whereas its metal complexes show Φ_F values up to 55 % at similar solution concentration. This observation can be attributed to the rigidification of the TPE skeleton upon metalation resulting in a restriction of the intramolecular rotation of the phenyl groups. Functionalization of the complexes [M₂ 2 b ](PF₆)₂ (M=Ag, Au) with terminal coumarin groups and subsequent photoirradiation yielded the complexes [M₂ 3 b ](PF₆)₂ (M=Ag, Au) bearing a new type of ligand with an unaffected TPE moiety.     

Free energy loss analysis of heterojunction solar cells

For the first time we present a free energy loss analysis (FELA) of heterojunction silicon solar cells (HSSC) to study the influence of the intrinsic buffer layer thickness (t_buffer) on the solar cell efficiency (η). The main advantage of the FELA is that the impact of various loss mechanisms can be directly expressed in absolute percentage of η. Furthermore, it is possible to extract the magnitude of every loss for each region of the solar cell. All quantities required to perform the FELA are obtained by the simulation software AFORS‐HET. The FELA yields an optimum efficiency of 21.24% for t_buffer ≈ 5 nm. The efficiency drop for t_buffer £ 5 nm is ascribed to a lower maximum usable generated power Φ_G(22.84% @ 2 nm, 23.98% @ 5 nm). Lower efficiencies for t_buffer ³ 5 nm are attributed to the increased transport loss of holes in the intrinsic buffer layer (0.05% @ 2 nm, 0.65% 8 nm). The η values yielded by the FELA are in agreement with the ones calculated by AFORS‐HET, demonstrating the applicability of the FELA to the HSSC concept. Therewith, we demonstrate that the FELA can be employed to obtain a deeper understanding of the HSSC concept. (© 2013 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)