Pyrolyse eclair de polyacrylonitriles entre 400 et 800°

Flash pyrolysis of radical and anionic polyacrylonitriles between 400 and 800° and in the absence of oxygen leads to various degradation products, the most characteristic being cyanhydric acid,. cyanogen, acrylonitrile and two dimers α-methyleneglutaronitrile and a cyanopicoline. Two important parameters have been studied: molecular weight ($\text{4 × 10}{}^3\text{<}\text{M}{}_{\mathrm{<mtext>w</mtext>}}\text{< 1·6 × 10}{}^6$) and branching density (0 < N/X < 0·6). At 400°, the yields in acrylonitrile and α-methylene glutaronitrile increase with branching density. All the experimental results may be interpreted on the basis of random chain scission, hydrogen transfer reactions and cyclization of the nitrile groups.     

Strong modulation of two-photon excited fluorescence of quadripolar dyes by (de)protonation

Two quadripolar dyes have been designed and synthesized that present large cross sections for two-photon excitation and whose fluorescence responds strongly to (de)protonation. These dyes are considered as prototypes of molecular pH probes for multiphoton fluorescence microscopy.     

Chiral discrimination of phenoxypropionic acid herbicide enantiomers on teicoplanin phase: methanol dependence and eluent pH consideration

The chiral recognition mechanism for a series of d,l phenoxypropionic acid herbicides (PPAs) on a teicoplanin stationary phase was investigated in reversed phase liquid chromatography (RPLC) over a wide range of mobile phase pH and column temperature. The effect of methanol on the enantiomeric separation was studied by varying its fraction (v/v) in the mobile phase. The thermodynamic data indicated that the chiral recognition was controlled by the interaction between the anionic form of the solute and the teicoplanin phase while those with the neutral form played a minor role. In addition, it was demonstrated that the enhancement of the separation factor observed as the methanol fraction increased in the mobile phase was enthalpically controlled owing to stereoselective binding interactions. Such behavior was used to optimize the chromatographic conditions for separation of PPAs herbicides on teicoplanin.     

Isolation and characterization of a polymeric lanthanum citrate

The first lanthanide citrate coordination polymer with the formula [La(Hcit)(H(2)O)](n) (Hcit(3-) = C(OH)(COO(-))(CH(2)COO(-))(2)) was prepared from La(2)O(3) and citric acid at pH = 2.2-2.5 under hydrothermal conditions at 120 degrees C. The compound was characterized by elemental analysis, IR, TG-DTA, and X-ray crystallography. It is thermally stable up to 158 degrees C and insoluble in common solvents. The compound crystallizes in the monoclinic space group C2/c with a = 16.765(3) A, b = 8.822(2) A, c = 14.048(3) A, beta = 120.64(3) degrees , and Z = 8. The structure consists of chains of La(III) cations bridged by O--C--O groups with pendant Hcit anions forming a pillar structure. The Hcit ligand is involved in six La--O bonds to five different La centers in a very compact 3D structure.     

Supercoiled circular DNA retention in nonequilibrium chromatography: viscosity and velocity dependence--behavior difference with proteins

This study demonstrates that the retention behavior of various circular double-stranded DNA molecules (3, 5, and 10 kb) increases over the entire flow-rate range (0.02-1.8 mL/min) at all the mobile phase viscosities (h). The transition between the two well-known nonequilibrium chromatography methods (slalom and hydrodynamic chromatography) is clearly visualized for proteins and does not appear for plasmids because of their strong compact structure. Also, the optimal conditions for F and h are determined to obtain the most efficient separation of these three plasmids in a minimum analysis time.     

Tunable resonance hyper-Raman spectroscopy of second-order nonlinear optical chromophores

Two-photon-resonant hyper-Raman spectra are reported for three "push-pull" conjugated organic chromophores bearing -NO(2) acceptor groups, two dipolar and one octupolar. The excitation source is an unamplified picosecond mode-locked Ti:sapphire laser tunable from 720 to 950 nm. The linear resonance Raman spectra of the same molecules are measured using excitation from the laser second harmonic. Excitation on resonance with the lowest-lying band in the linear absorption spectrum yields nearly identical resonance Raman and resonance hyper-Raman spectra. However, excitation into a region that appears to contain more than one electronic transition gives rise to different intensity patterns in the linear and nonlinear spectra, indicating that different transitions contribute differently to the one-photon and two-photon oscillator strength. The promise of the hyper-Raman technique for examining electronic transitions that are both one- and two-photon allowed is discussed.     

Variantes de mycosides caracterisees par des residus glycosidiques substitues par des chaines acyles–I: Spectres de masse des mycosides G′ et A′ peracetyles

Mass spectra of peracetylated mycosides G′ and A′ are characterised by rearranged oxonium ions, corresponding to deoxysugars which have lost an acyl chain by fragmentation in the mass spectrometer. The main carboydrate constituent of mycoside G′ is a deoxysugar with one acyl chain and a methyl group. Mycoside A′ contains deoxysugars with one acyl chain and 0, 1 or 2 methyl groups. Deoxysugars with no acyl chains and one (G′, A′) or two (A′) methyl groups are also present. The mass spectra indicate that the acyl chains might be of the mycolic type: Peaks which might correspond to a fragmentation on both sides of the methyl branching are present and the CH⁺˙?C? C₂₂H₄₅ fragment, found in the spectrum of paracetylated mycoside A′ is characteristic of the branched chain. The highest peaks (m/e 1072 and 1100) in the spectrum of paracetylated mycoside A′ can be due to a mycolic chain after loss of acetic acid, methanol and H (l) on loss of acetic acif and H (m). The nature and abundance of the mycocerosic acids which esterify the aglycones can be deduced from the same spectra, as well as the structure of these aglycones which has been established previously by degradation and mass spectrometry. In order of decreasing abundance, C₂₇ and C₂₄ mycocerosic acids are present in mycoside G′, and C₂₉, C₃₂, C₃₂, C₃₀ and C₂₇ mycocerosic acids are found in mycoside A′.     

Umsetzung von Di(tert-butyl)- und Diphenyldiazomethan mit 1,3-Thiazol-5(4H)-thionen: Isolierung und Kristallstruktur des primären Cycloadduktes

Reaction of Di(tert-butyl)- and Diphenyldiazomethane and 1,3-Thiazole-5(4H)-thiones: Isolation and Crystal Structure of the Primary Cycloadduct Reactions of diazo compounds with C?S bonds proceed via the formation of thiocarbonyl ylides, which, under the reaction conditions, undergo either 1,3-dipolar cycloadditions or electrocyclic ring closer to thiiranes (Scheme 1). With the sterically hindered di(tert-butyl)diazomethane ( 2c ), 1,3-thiazole-5(4H)-thiones 1 react to give spirocyclic 2,5-dihydro-1,3,4-thiadiazoles 3 (Scheme 2). These adducts are stable in solution at ?20°, and they could be isolated in crystalline form. The structure of 3c was established by X-ray crystallography. In CDCl₃ solution at room temperature, a cycloreversion occurs, and the adducts of type 3 are in an equilibrium with 1 and 2c . In contrast, the reaction of 1 with diphenyldiazomethane ( 2d ) gave spirocyclic thiiranes 4 as the only product in high yield (Scheme 3). The crystal structure of 4b was also determined by X-ray analysis. The desulfurization of compounds 4 to 4,5-dihydro-5-(diphenylmethylidene)-1,3-thiazoles 5 was achieved by treating 4 with triphenylphosphine in boiling THF. The crystal structure of 5f is shown.     

Resonance hyper-Raman excitation profiles and two-photon states of a donor-acceptor substituted polyene

Resonance Raman and resonance hyper-Raman spectra and excitation profiles have been measured for a "push-pull" donor-acceptor substituted conjugated polyene bearing a julolidine donor group and a nitrophenyl acceptor group, in acetone at excitation wavelengths from 485 to 356 nm (two-photon wavelengths for the nonlinear spectra). These wavelengths span the strong visible to near-UV linear absorption spectrum, which appears to involve at least three different electronic transitions. The relative intensities of different vibrational bands vary considerably across the excitation spectrum, with the hyper-Raman spectra showing greater variation than the linear Raman. A previously derived theory of resonance hyper-Raman intensities is modified to include contributions from purely vibrational levels of the ground electronic state as intermediate states in the two-photon absorption process. These contributions are found to have only a slight effect on the hyper-Rayleigh intensities and profiles, but they significantly influence some of the hyper-Raman profiles. The absorption spectrum and the Raman, hyper-Rayleigh, and hyper-Raman excitation profiles are quantitatively simulated under the assumption that three excited electronic states contribute to the one- and two-photon absorption in this region. The transition centered near 400 nm is largely localized on the nitrophenyl group, while the transitions near 475 and 355 nm are more delocalized.