Photobinding of ketoprofen in vitro and ex vivo

Ketoprofen (KP), a non-steroidal anti-inflammatory drug of the 2-aryl propionic class, has been shown to produce photoallergic side effects as well as cutaneous photosensitizing properties that induce other phototoxic effects. In the present study we investigated photobinding of ketoprofen to both human serum albumin (HSA), a model protein, and to ex vivo pig skin and its photodegradation. Results demonstrate that photoadduct formation and photodegradation progressively increased with irradiation time where they reach a maximum. Maximum photobinding to the viable layer of the epidermis was about 7-8% of the initial radiolabelled KP added, in the region of 15-30 min UV irradiation. These results were comparable to in vitro results that were seen with photobinding of KP to HSA; in this case, the quantity of covalently bound material was approximately 10% of the initial, after a maximum of 18 min irradiation. It was found by HPLC analysis that the KP decrease is accompanied by an increase of the corresponding photoproduct, decarboxylated ketoprofen (DKP). The yield of DKP reaches a maximum at around 15 min. DKP appears to play an important role in vitro and ex vivo, being the major photoproduct and responsible for the photobinding process. Using micro-autoradiographical techniques we investigated the penetration and distribution of ketoprofen in ex vivo pig skin in greater detail. It was apparent that percutaneous absorption was taking place and that most of the ketoprofen was predominately localised in fibroblasts in the papillary dermis. No other specific localisation within the skin architecture was identified. Although there were differences in the quantities of bound ketoprofen within the different layers of the skin, these levels did not appear to correlate with irradiation time.     

Calculation of χ)(3) in He including configuration interaction for XUV photons

We calculate the third-order susceptibility in He for photon energies from 19.5 eV to 24.5 eV in a configuration-interaction calculation, and discuss the role of autoionizing states as a means of enhancing harmonic generation.     

Determination of platinum, palladium, and gold in a silver assay bead by atomic absorption spectrophotometry

Summary A procedure is given for the atomic absorption determination of platinum, palladium and gold in silver beads. Interferences by coexisting ions usually found in the parting solution could be eliminated by addition of 1% of lanthanum. The lowest working ranges in which it is possible to obtain results comparable in accuracy to those from a good spectrophotometric determination are estimated for each metal. (1 ppm Pd, 1 ppm Au, 5 ppm Pt). The results of several determinations using the proposed procedure to analyse silver assay beads are given.

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Bestimmung von Platin, Palladium und Gold in dokimastischen Silberperlen durch Atomabsorptions-Spektrophotometrie

Zusammenfassung Störungen durch in der Scheidelösung vorhandene Begleitionen konnten durch Zusatz von 1% Lanthan verhindert werden. Die unteren Grenzen für eine genaue Bestimmbarkeit wurden festgelegt (1 ppm Pd, 1 ppm Au, 5 ppm Pt) und Ergebnisse mehrerer Beleganalysen mitgeteilt.

     

Magnetic behavior of copper diethyldithiocarbamate at low temperatures: A reinvestigation

The title compound, Cu(S₂CNEt₂)₂, behaves at low temperatures (1–20 K) as a normal spin-1/2 molecule, with 〈g〉 =2.06 and the Curie-Weiss θ = +0.25 K. This result contradicts an earlier investigation that led to the suggestion that the crystallographically-occurring dimers are coupled ferromagnetically.     

On the thin cell method in time domain spectroscopy

A simple physical picture is given of Fellner-Feldegg's thin cell method in time domain spectroscopy. From this picture an accurate analytical relation is derived for the total reflection coefficient.     

Vibrational Population of Hydrogen Molecules Excited by an RF Discharge in an Expanding Thermal Arc Plasma as Determined by Emission Spectroscopy

This work is devoted to the determination of the vibrational population of hydrogen molecules in the ground and excited electronic states from the analysis of visible spectra of the H₂ molecules excited by an RF discharge in an expanding thermal arc plasma. Comparison of the experimental results on relative electron-impact excitation cross sections for the transition H₂(X¹Σ, υ⁰ = 0)→ H₂(d³II_u, υ′) with other experiments, and with calculations based on the Franck-Condon principle, shows good agreement. This means, that for plasma under investigation: 1) in the ground electronic state H₂(d³II_u,υ′), only the lowest vibrational level with υ⁰ = 0 is significantly populated, and 2) direct electron exictation of H₂(d³II_u, υ′, υ′) state from the ground state H₂(X¹Σ, υ⁰ = 0) dominates.     

CW diode pumping and FM mode locking of a Nd: KGW laser

We have demonstrated cw diode end pumping of Nd: KGW, a novel solid-state gain medium, with up to 30% conversion efficiency into near-TEM₀₀ (M² < 1.05) output at = 1.067 µm for a pump level of 2.7 W. The slope efficiency was limited by intracavity reflections to 36%; however, direct comparison to a similar Nd:YAG laser indicates the same intrinsic slope efficiency of 60%. FM mode locking of this laser at 200 MHz has produced 12 ps pulses (compared to 16 ps for Nd: YAG), although an intracavity etalon was required. Considerable reduction in pulse width is possible (the line width limit is 0.5 ps) but different techniques may be necessary. Spatial hole burning was evident in both the 120 GHz free-running spectrum and the etalon-limited mode-locked spectrum.     

Close coupling results for inelastic collisions of NH3 and Ar. A stringent test of a spectroscopic potential

We have calculated state-to-state total cross sections for rotational excitation and inversion of NH3 by collisions with Ar using the close coupling method. The Ar-NH3 interaction potential has been obtained from a fit to the spectrum of this van der Waals molecule. The calculated cross sections agree to within about 30% with the measured values; the estimated error in the latter is 10% to 20%.