A novel calibration procedure for trace analytical measurements: application to the analysis of polybrominated diphenyl ethers by GC-MS

The measurement of polybrominated diphenyl ethers (PBDEs) by gas chromatography-mass spectrometry (GC-MS) is highly challenging due to existence of the analytes at trace levels and the instability of the higher molecular weight PBDEs. These properties make accurate analysis especially problematic when utilising a low-resolution 'bench-top' GC-electron impact (EI) mass spectrometer. We discuss the problems associated with the analyses of PBDEs on these common GC-EI-MS systems and present a novel approach to calibration in these circumstances. We propose that this 'mixed calibration procedure' allows analyses to be performed that would not be possible using traditional calibration techniques, and that the procedure may be applied to a wide range of applications throughout analytical science.     

Analysis of monoethanolamine by derivatization with Marfey's reagent and HPLC

A sensitive and selective method for determining the residual monoethanolamine in a developmental drug substance is developed and validated. Marfey's reagent, which is commonly used for the chiral analysis of amino acids, is reacted with the primary amine group of monoethanolamine and then analyzed by high-performance liquid chromatography-UV at 340 nm. Quantitation is performed by a standard addition method by preparing drug substance samples with added monoethanolamine ranging from 0.25-1.0 microg/mL (equivalent to 12.5-50 ppm with respect to the drug substance). The method performance is evaluated for linearity, specificity, detection and quantitation limits, accuracy, precision, and sample stability. The method is linear from 0.25-1.0 microg/mL with a coefficient of determination (r(2)) > 0.95. The accuracy and precision obtained is 105.5 +/- 4.8% (n = 3). The limits of detection and quantitation are 0.03 and 0.10 microg/mL, respectively. Instrument precision (% relative standard deviation of six injections of a derivatized 0.5 microg/mL monoethanolamine solution on two separate days) is >/= 2.0%. This method is suitable for the determination of monoethanolamine at the 25 ppm level in drug substance.     

Mukaiyama addition of (trimethylsilyl)acetonitrile to dimethyl acetals mediated by trimethylsilyl trifluoromethanesulfonate

(Trimethylsilyl)acetonitrile reacts smoothly with dimethyl acetals in the presence of stoichiometric trimethylsilyl trifluoromethanesulfonate (TMSOTf) to yield β-methoxynitriles. The ideal substrates for this reaction are acetals derived from aromatic aldehydes. Elimination to the corresponding α,β-unsaturated nitriles is observed as the major product in the case of electron-rich acetals. A mechanistic hypothesis that includes isomerization of the silylnitrile to a nucleophilic N-silyl ketene imine is presented.     

Synthesis of N-acyl-N,O-acetals from N-aryl amides and acetals in the presence of TMSOTf

Secondary amides undergo in situ silyl imidate formation mediated by TMSOTf and an amine base, followed by addition to acetal acceptors to provide N-acyl-N,O-acetals in good yields. An analogous, high-yielding reaction is observed with 2-mercaptothiazoline as the silyl imidate precursor. Competing reduction of the acetal to the corresponding methyl ether via transfer hydrogenation can be circumvented by the replacement of CY₂NMe with 2,6-lutidine under otherwise identical reaction conditions.     

Systematic investigation of absorption, fluorescence and laser properties of some p- and m-oligophenylenes

Absorption, fluorescence and laser properties of ten selected aromatic compounds from the oligophenylene family are studied experimentally at room temperature (293 K). The first eight compounds are arranged in such way that odd numbered compounds reveal 1Lb --> 1A fluorescence, while even numbered compounds show 1La --> 1A fluorescence. All compounds are family related in pi-structure and are of the same degree of planarity and rigidity. The quantum yield of fluorescence, gamma, and the decay times, tau(f), of non-deaerated and deaerated cyclohexane solutions are measured. The oscillator strength, f(e), the fluorescence rate constant, Kf, natural lifetimes, tau(o)T, and intersystem crossing rate constant, K(ST), are calculated. The lowest 1Lb and 1La singlet and 3La, triplet (77 K) levels are determined. Investigations showed that transition from a polyphenyl molecule which shows 1La --> 1A fluorescence to a family related in the pi-structure molecule which reveals the 1Lb --> 1A fluorescence is accompanied by certain changes in all the fluorescence parameters. This indicates that gamma decreases, tau(f) increases, Kf and the FWRE of the fluorescence spectrum decrease. Moreover, K(ST) also decreases, sometimes very significantly. The decrease in the K(ST) value is explained by the fact that matrix elements of the spin-orbit coupling of the S alpha and Ti states are much lower in value than analogous elements of the spin-orbit coupling of Sp and Ti states. It is shown that all p-polyphenyles exhibit excellent laser action, while m-polyphenyles do not produce laser oscillation under any conditions. The values of K(ST) and other fluorescence parameters measured can be used for various practical purposes and theoretical considerations.     

Multimodal hard X‐ray imaging of a mammography phantom at a compact synchrotron light source

The Compact Light Source is a miniature synchrotron producing X‐rays at the interaction point of a counter‐propagating laser pulse and electron bunch through the process of inverse Compton scattering. The small transverse size of the luminous region yields a highly coherent beam with an angular divergence of a few milliradians. The intrinsic monochromaticity and coherence of the produced X‐rays can be exploited in high‐sensitivity differential phase‐contrast imaging with a grating‐based interferometer. Here, the first multimodal X‐ray imaging experiments at the Compact Light Source at a clinically compatible X‐ray energy of 21 keV are reported. Dose‐compatible measurements of a mammography phantom clearly demonstrate an increase in contrast attainable through differential phase and dark‐field imaging over conventional attenuation‐based projections.     

Hard X‐ray phase‐contrast imaging with the Compact Light Source based on inverse Compton X‐rays

The first imaging results obtained from a small‐size synchrotron are reported. The newly developed Compact Light Source produces inverse Compton X‐rays at the intersection point of the counter propagating laser and electron beam. The small size of the intersection point gives a highly coherent cone beam with a few milliradian angular divergence and a few percent energy spread. These specifications make the Compact Light Source ideal for a recently developed grating‐based differential phase‐contrast imaging method.     

Thermally-induced structural and electrical effects in GeTe-based amorphous alloys

The thermal, structural electrical properties of bulk glasses based on GeTe compositions near the binary eutectic, Ge₁₅Te₈₅, are studied. Information regarding the non-crystalline state and the transformation from the non-crystalline to the crystalline state is reported. The particular alloys studied represent binary (Ge₁₇Te₈₃), ternary (Ge₁₅Te₈₀As₅) and quaternary (Ge₁₅Te₈₁Sb₂S₂) compositions. Structural information is obtained using X-ray diffraction techniques and density measurements. Thermal data are reported from differential scanning calorimetry (DSC), thermogravimetry (TGA) and mass spectrometry results. The electrical conductivity is measured as a function of temperature and, on the ‘as-prepared’ glasses, shows semi-conducting behavior with activation energies, E, of 0.43–0.48 eV. DSC, TGA and X-ray powder diffraction patterns indicate the samples crystallize as Te and GeTe in a two-step process, and melt at the binary eutectic temperature. The binary vaporizes as Te and GeTe in a two-step process. GeTeAs and GeTeSbS vaporize by essentially the same mechanism, with As evaporating (<300°C) before the Te, and Sb and S evaporating (420–480°C) after the Te but before GeTe. The results show that the properties of the bulk ‘as-prepared’ glasses are strikingly similar. Thermally-induced changes in the structural and electrical properties of bulk samples have been examined following a series of anneals (5 h, vacuum) at temperatures from 111°C to 190°C (glass transition temperature $\text{?125?133°}\text{C}$; crystallization temperature $\text{?206?228°}\text{C}$ as determined by DSC). DSC, TGA and mass spectrometry results have been correlated to electrical and structural changes. Results show that crystalline Te nucleates at the surface and forms a conductive surface layer. The conductivity of this surface layer is nearly temperature independent with E ≈ 10^?2 eV for all three alloys. Crystallization and the associated electrically conductive regions extend into the bulk material with further annealing. In these disordered alloys the additives As and Sb + S apparently do not act as electrical dopants in the sense of affecting the conductivity activation energy. The additives Sb + S however do retard crystallization of GeTe. The secondary crystallization product, GeTe, apparently changes the conduction mechanism to either a metallic or degenerate semiconductor type behavior.     

Determination of oxalate in pharmaceutical matrices by indirect photometric chromatography

An indirect photometric ion chromatography method is developed for the quantitation of oxalate in typical pharmaceutical matrices. The column/mobile phase conditions used represent a trade off between resolving power and sensitivity and results in an assay with a total analysis time of less than 9 minutes. Method response is linear between concentrations of 10 to 80 ppm oxalate. The limit of quantitation is roughly 5 ppm. Precision in the range of 30 to 80 ppm is better than 1.0% RSD of replicate injections, and the accuracy in a variety of matrices is 100 +/- 2%. The method is quite rugged and meets rigorous suitability requirements even after 500 injections. Although the assay can be used to quantitate citrate as well, the retention time is relatively long (20 minutes) and sensitivity is limited due to the broadness of the peak.