Use of 13C to monitor soil organic matter transformations caused by a simulated forest fire

Soil organic matter (SOM) transformations caused by heating were analyzed using the stable carbon isotope (13)C as a tracer to follow C mineralization dynamics and C transfers between different organic compartments. A (13)C-labelled soil, obtained by incorporation of (13)C-enriched Lolium perenne phytomass into a pine forest soil, was heated for 10 min at 385 degrees C to reproduce conditions typical of a forest fire and changes in total C content, potential C mineralization activity and C distribution between the different soil organic fractions were determined. Changes caused by heating on the potential soil C mineralization, determined by laboratory aerobic incubation, reveal alterations to the SOM biodegradability; some stabilized SOM showed an increase in biodegradability, whereas less stabilized SOM became more resistant to microorganisms. Chemical fractionations of SOM allowed us to monitor changes in its composition. As a consequence of heating, the less polymerized humic fractions were the most strongly affected, with the total disappearance of fulvic acids. A significant increase in the quantity and degree of polymerization of the humic acids at the expense of other more (13)C-enriched substances was also found. Finally, a large decrease in humin was observed, its solubilizable part disappearing completely, probably as a consequence of the incorporation of the byproducts into the free organic matter fraction.     

Columnar mesomorphic organizations in cyclotriphosphazenes

A synthetic strategy has been developed to prepare cyclotriphosphazenes that bear polycatenar aromatic esters as promesogenic units linked to phosphorus atoms. The microsegregation of the rigid and flexible parts of the system and the space-filling properties are the driving forces that determine the kind of mesomorphism exhibited by the organocyclotriphosphazenes. Mesogenic units that contain only one terminal alkyl chain give rise to calamitic mesomorphism, since the molecules are arranged to give a cylindrical superstructure with the aromatic promesogenic cores elongated in a manner approximately perpendicular to the cyclotriphosphazene ring. On the other hand, mesogenic units that contain three long terminal chains exhibit columnar mesophases. In this case, a discotic structure consisting of promesogenic cores arranged approximately parallel to the cyclotriphosphazene ring can explain the columnar organization. The X-ray diffraction patterns corresponding to the Col(h) mesophase of the cyclotriphosphazene with dodecyloxy chains (8) indicate the presence of helical ordering, which was confirmed for a homologous compound bearing stereogenic centers on two of the terminal chains (11). All of the synthesized phosphazenes show a high thermal stability.     

A validated liquid chromatographic tandem mass spectrometric method for the determination of mirtazapine and demethylmirtazapine in human plasma: application to a pharmacokinetic study

A new liquid chromatographic tandem mass spectrometric method for the determination of mirtazapine and demethylmirtazapine in human plasma has been developed and fully validated. The article describes in detail the bioanalytical procedure and summarizes the validation results obtained. The samples were extracted using liquid-liquid extraction with a mixture of 1-chlorobutane/isopropanol/ethyl acetate (88:2:10, (v/v/v)). The chromatographic separation was performed on a reversed-phase XTerrra MS C₈ column ( i.d.; 3.5 μm particle size) using a mobile phase consisting of 0.010 M ammonium formate (pH 7.8) and acetonitrile (35:65, (v/v)), pumped at a flow rate of 0.80 ml min⁻¹. The analytes were detected using a Finnigan LCQ advantage ion-trap mass spectrometer with positive electrospray ionization in selected reaction monitoring (SRM) mode. Tandem mass spectrometric detection enabled the quantitation of both compounds down to 0.10 ng ml⁻¹. Calibration graphs were linear (r better than 0.990, n=11), in concentration ranges 0.10 to 200 ng ml⁻¹ for mirtazapine demethylmirtazapine. The intra- and inter-day R.S.D. values were less than 14.8 and 16.6% for mirtazapine and demethylmirtazapine, respectively. The method was successfully applied to a kinetic study in order to assess the main pharmacokinetic parameters of mirtazapine and demethylmirtazapine.     

4-Currents in relativistic quantum chemistry

Some topics in relativistic quantum chemistry are reviewed with special emphasis on 4-currents and 4-potentials. It is shown that, both in molecular quantum theory and in solid-state physics, calculations can include relativistic and magnetic effects by means of 4-currents without an excessive increase in complication, provided that 4-component Dirac spinors are used rather than the Pauli approximation. © 1993 John Wiley & Sons, Inc.     

CHLORPROMAZINE AND PROTRIPTYLINE PHOTOTOXICITY: PHOTOSENSITIZED, OXYGEN INDEPENDENT RED CELL HEMOLYSIS

Abstract—Red blood cell lysis photosensitized by chlorpromazine and protriptyline was investigated. Oxygen independent sensitized photohemolysis was observed with both compounds. When chlorpromazine and protriptyline were irradiated in the absence of red cells, both formed photoproducts which lysed red cells. These results indicate that chlorpromazine and protriptyline represent a new mechanistic class of phototoxic compounds which photosensitize membrane disruption by oxygen independent processes.     

Geometry, phase stability, and electronic properties of isolated selenium chains incorporated in a nanoporous matrix

We report the fabrication process of isolated one-dimensional Se chains incorporated in the matrix of AlPO4-5 single crystals and the experimental investigation of the geometry, phase stability, electronic properties, and electron-phonon coupling effect of these Se chains. The structure of the helical Se chains inside the channels is discussed on the basis of X-ray scattering measurements. Thermal analysis and temperature-dependent micro-Raman measurements show that Se single chains are flexible and can convert from a weak distorted phase into another phase with strongly disordered structure ("melting" state) around 340 K. Since the electrons are confined in the one-dimensional channels, the absorption band of the Se chain is obviously blue shifted compared with that of trigonal Se. With increasing temperature, this band shifts linearly to the lower energy side, in sharp contrast to the nonlinear temperature coefficient of trigonal Se, which is attributed to the greatly diminished interchain interaction and the weakening of the electron-optical phonon coupling in a low-dimensional system. In the vicinity of the absorption band, both first-order and second-order Raman signals for the Se chain are enhanced, due to the strong electron-phonon coupling when the excitation laser energy matches the electronic transition in isolated Se chains.     

The crystal structure of the inclusion complex of cyclomaltoheptaose (β-cyclodextrin) with 3,5-dimethylbenzoic acid

The crystal of theCD-3,5-dimethylbenzoic acid inclusion complex is triclinicP1 witha=15.707(3),b=15.694(3),c=15.999(3) Å, =101.502(5),=101.557(5), =103.805(4)°,V=3624 ų, andZ=1. Two crystallographically independentCD molecules form a dimer by means of hydrogen bonds between secondary hydroxyl groups in which disordered guest molecules in six orientations are accommodated. In two of them the guest molecules are situated at the dimer interface, their carboxyl groups interacting with the carboxyl groups of two other guest orientations that are found on either side of the monomer cavity. In the two last orientations the guest molecules enter the monomer cavities in an opposite sense with the carboxyl groups protruding from the primary side and are stabilized by cyclodextrin hydroxyl groups. A dense water network is formed in the interdimer space consisted of 18.2 water molecules distributed over 24 sites. Supplementary Data relating to this article are deposited with the British Library as Supplementary Publication No. SUP 82175 (61 pages).Dedicated to Professor József Szejtli.     

Electronic states and nature of bonding in the molecule YN by all-electron ab initio CASSCF calculations

In the present work, we present results of all-electron ab initio CASSCF calculations of nine electronic states of the molecule YN. Also reported are the spectroscopic constants derived on the basis of the calculated potential energies. The predicted electronic ground state is ¹∑⁺, and this state is found to be separated from the excited states ³∑⁺, ³Π, and ¹Π by 5177, 9290, and 9915 cm^?1, respectively. The chemical bond in the YN molecule is polar with charge transfer from Y to N, giving rise to a dipole moment of 8.19 Debye at 3.3 au in the ¹∑⁺ ground state is basically a double bond composed of two π bonds. The dissociation energy of the YN molecule has been derived as 4.59 eV. © 1993 John Wiley & Sons, Inc.     

Development and validation of a high-performance liquid chromatographic method for the analysis of antioxidative phenolic compounds in fennel using a narrow bore reversed phase C18 column

A simple high-performance liquid chromatography (HPLC) method for the separation and quantitative determination of the main antioxidant phenolic compounds from bitter fennel, Foeniculum vulgare, was developed. The use of a narrow bore reversed phase (RP) C₁₈ column and an acidic mobile phase enabled ten compounds (caffeoylquinic acids, dicaffeoylquinic acids, flavonoids and rosmarinic acid) to be separated within a 40 min time analysis. The method was validated to demonstrate its selectivity, linearity, precision, accuracy and robustness. In addition, some parameters were studied to optimize the complete extraction of the phenolic compounds. The method was applied to the evaluation of three different fennel materials: distilled and non-distilled aerial parts, as well as defatted fruits. Distilled fennel was found to contain a higher proportion of antioxidant phenolic compounds than the non-distilled plan material.     

The dissociation dynamics of He...I 35Cl(B,v'=2,3) complexes with varying amounts of internal energy

The He...I (35)Cl intermolecular vibrational levels with n'=0-6 that are bound within the He+ICl(B,v'=3) potential [A. B. McCoy, J. P. Darr, D. S. Boucher, P. R. Winter, M. D. Bradke, and R. A. Loomis, J. Chem. Phys. 120, 2677 (2004)] are identified in laser-induced fluorescence experiments performed at very low temperatures within a supersonic expansion. Comparisons of the positions and intensities of these lines with the excitation spectra, calculated using potential surfaces to describe the interactions between the helium atom and ICl in its ground and excited state, assist in the assignments. Based on these comparisons the excited state potential was rescaled so that the experimental and calculated J'=0 energies agree to within the experimental uncertainties for all but the lowest, n'=0, intermolecular level. Two-laser, action, and pump-probe spectroscopy experiments indicate that the bound He...I (35)Cl(B,v'=3) intermolecular vibrational levels undergo vibrational predissociation forming rotationally excited I (35)Cl(B,v'=2,j') products with distributions that depend upon the initial intermolecular vibrational level excited. Action spectra recorded in the ICl B-X, 2-0 region while monitoring the Deltav=0, I (35)Cl(B,v'=2) channel reveal two additional dissociation mechanisms for the He...I (35)Cl(B,v') excited state complexes: rotational predissociation of discrete metastable states lying slightly above the He+I (35)Cl(B,v'=2) asymptote and direct dissociation that occurs when the linear conformer is excited to the continuum of states above the same asymptote. The rotational predissociation pathway forms I (35)Cl(B,v'=2,j') products in all of the rotational states energetically accessible. The direct dissociation mechanism yields very cold rotational product state distributions; for instance, the average rotational energy in the product state distribution measured when the linear complexes are prepared 20 cm(-1) above the dissociation limit is only 1.51 cm(-1), representing only 7.6% of the available energy.