Infrared photolysis of C2F4S2: a comparison of multiphoton dissociation models

Infrared multiphoton dissociation of the planar ring compound

has been shown to yield two CF₂S molecules. The threshold for dissociation using the R(16) transition of the 9.6 μm CO₂ laser is 0.12 J/cm². At fluences above 1 J/cm³ dissociation is accompanied by the emission of light in the 300–750 nm region. The fractional dissociation per pulse and the average energy deposition have been measured as functions of laser fluence, laser wavelength, C₂F₄S₂ pressure, and added argon pressure. The variations of the fractional dissociation with fluence and absorbed energy are compared to the predictions of two models. The first model is based on the assumption of a Planck distribution for the dissociating C₂F₄S₂ molecules, while the second is based on a rate equation approach to the dissociation. Both models predict that the dissociating parent compound has a rather broad vibrational distribution.     

Multiple infrared photon dissociation of vinyl chloride

Dehydrohalogenation of vinyl chloride, to form acetylene and HCL, is produced by irradiation with infrared laser pulses in the 9–11 μm region. The acetylene itself is broken down to yield diacetylene and elemental carbon and hydrogen when irradiated by focussed laser pulses. Initial excitation into vibrational modes of different symmetry appears to be about equally effective in converting absorbed energy to chemical reaction. The results are analyzed in terms of several models for multiple infrared photon dissociation; threshold energies of 20· 50 J/cm² are deduced.     

Validation of an analytical LC-MS/MS method in human plasma for the pharmacokinetic study of atomoxetine

This study aimed to validate a sensitive and reliable analytical method for the pharmacokinetic study of atomoxetine in human plasma by liquid chromatography-electrospray ionization-tandem mass spectrometry. Metoprolol was used as an internal standard. After liquid-liquid extraction with methyl t-butyl ether, the supernatant was evaporated. The residue was then reconstituted and an aliquot was injected into the high performance liquid chromatographic system. Separation was performed on a Phenomenex Luna C₁₈ column (2.0 mm × 100 mm, 3 μm particles) with a mobile phase of 10 mM ammonium formate buffer: methanol = 10: 90 (v/v). Tandem mass spectrometry was performed in the electrospray ionization positive ion mode using the multiple reaction monitoring mode for quantification. The mass transition pairs of m/z 256 → 44 for atomoxetine and m/z 268 → 116 for the internal standard were used. The flow rate of the mobile phase was 0.25 mL/min and the retention times of atomoxetine and the internal standard were found to be 1.0 and 0.9 min, respectively. The calibration curve for atomoxetine was linear in the concentration range of 1–750 ng/mL (r ² = 0.9992) with a lower limit of quantification of 1 ng/mL. The mean accuracy for atomoxetine was 93–102%. The coefficients of variation (precision) in the intra- and inter-day validation for atomoxetine were 4.0–6.8 and 1.1–9.6%, respectively. The pharmacokinetic parameters of atomoxetine were evaluated after administration of a 40-mg single oral dose to twelve healthy male volunteers. The mean AUC_{0–24 h}, C _max, T _max and T _1/2 for atomoxetine were 1.9 ± 0.8 μg h/mL, 0.34 ± 0.11 μg/mL, 1.0 ± 0.5 h and 3.9 ± 1.3 h, respectively.     

The spectrophotometric determination of nitrate in natural waters,with particular reference to sea-water

Nitrate can be reduced to nitrite in good yield by means of hydrazine in alkaline solution; the reaction is promoted by catalytic quantities of copper. The authors have established the optimum conditions for tlie reduction and applied the method to the determination of nitrate in fresh waters and in sea-waters. The nitrite formed is determined by Mellon and Rider's modification of the Griess-Ilosvay procedure. The reduction with hydrazine is carried out in the presence of 0.25 p.p.m. of copper at pH 9.6 in a solution buffered with sodium phenate. It is complete within 24 hours at room temperature. The method will detect ca. 0.3 μg NO₃$\text{N}\text{l}$ and gives a standard deviation of ca. 2% in the range 20-600 μg NO₃-$\text{N}\text{l}$. Up to 60 determinations can be made per 6 hour working period. The interference of nitrite has been investigated. Ammonium salts, urea, and amino acids do not interfere, at the concentrations at which they occur in sea-water.It is preferable to analyse samples immediately after collection, but if this is not possible, they should be filtered, sterilized with 2 p.p.m. of mercuric chloride and stored in glass containers.     

IR laser-induced decomposition of volatile uranyl complexes. I. Analysis of molecular beam depletions

A rigorous analytical procedure is presented for the fluence dependence of molecular beam depletions due to a pulsed gaussian laser profile. The procedure has been applied to depletion data for the molecules UO₂L₂B, where L = (CF₃CO)₂CH and B = tetrahydrofuran, trimethylphosphate, triethylphosphate and tributylphosphate. The parent ion (UO₂L₂B⁺) depletions are satisfactorily modelled by an initial rapid linear dependence on fluence, saturating at ≈ 0.5–0.65, much lower than previously believed. With depletion of this ion assigned to an initial isomerization, fragment ion (UO₂LB⁺) depletions have been analysed to yield estimates of the overall dissociation yield. For B = trimethyl-, triethyl- and tributylphosphate, excitation in the phosphate CO region at 9.4 μm appears to yield more efficient dissociation than excitation in the UO₂ asymmetric stretch at 10.6 μm as in the latter case there is a loss of interaction between the laser and isomerized molecules. On the timescale of the measurements, the same dissociation yield appears to require more energy deposited as the molecules become more complex.     

Megawatt infrared laser photochemistry of ketene

Multiphoton laser-induced decomposition is reported here for photolysis ketene with 9.260 μm radiation from a pulsed CO₂ TEA laser. Chemical end products of this photolysis were primarily H₂ and CO. Visible chemiluminescence, attributed to C₂ Swan band emission, was observed during the first ≈ 1 μs following photolysis. A collision-assisted dissociation, followed by rephotolysis of the transient products, is proposed to account for the results.     

Correlation of SiO x layer thickness and properties of BOPP/SiO x composite films with spin coating process parameters

The effects of the spin coating process parameters on the thickness of the SiOx layer of the BOPP/SiOx composite film were investigated. When the concentration of tetraethoxysilane (TEOS) increased from 12.5 vol% to 55% vol%, the SiOx thickness increased from about 80 nm to 470 nm. In the sol time range of 1.5 h to 5 h the SiOx layer thickness reached a maximum at about 4 h and the change of the thickness roughly matched the change of the silica colloidal sphere sizes in sol. When the spin-coating speed of the dispensing stage increased from 450 r/min to 500 r/min, the SiOx layer thickness drastically decreased from about 1.67 μm to 400 nm. While the spin-coating speed of the thinning and drying stage went up to 1200 r/min, the SiOx layer thickness was in the range of 330 nm to 390 nm. It was also found that the SiOx layer thickness was almost increased linearly from about 500 nm to 1.02 μm with the ratio of the commercial silica colloidal to the TEOS from 0.2 to 1.0. The water contact angles decreased to about 23.0° for the BOPP/Si-Sol composite film with 1.67 μm SiOx layer and about 4.0° for the BOPP/mixing Si-Sol composite film with 1.02 μm SiOx layer. Compared to BOPP, the light transparency of the BOPP/Si-Sol composite films decreased by about 5.5% with the SiOx layer from about 80 nm to 1.67 μm and by 7.0% for the BOPP/mixing Si-Sol composite film with the SiOx layer from about 350 nm to 1.02 μm respectively.     

Adhesion strength of filled polyaluminosilicates on aluminum surface

Study of the adhesion of coatings based on polyaluminosilicates of dendrimer structure, deposited on an aluminum surface of complex morphology with roughnesses R _a = 0.05–11.30 μm, demonstrated that the adhesion strength of the sample with R _a = 11.30 μm is 16 times that of a samples with a polished surface (R _a = 0.05 μm) and 2.3 times that of the coating deposited on the surface produced by microarc oxidation. It was demonstrated that the values obtained for the work of adhesion are well correlated with the parameters of profilograms, which is particularly important for choosing the composition of coatings and prognosticating their adhesion under working conditions.     

Ion decomposition versus molecular size probed by vacuum ultraviolet photoionization

The molecular size dependence of primary fragmentation is studied for a series of β -naphthyl esters having alkyl chain lengths from C2 to C18. The esters are vaporized at a known ftemperature and ionized by coherent vacuum ultraviolet radiation at 10.5 eV. The photoionization wavelength is energetic enough to cause both metastable and nonmetastable primary fragmentation to m / z 144, but not energetic enough to cause secondary fragmentation to m / z 115 or 116. Under these conditions, the ratio of the nonmetastable-to-metastable daughter ion current, D/m _D ^′ is expected to give a rough indication of the average parent ion dissociation rate. The D / m _D ratio decreases with increasing molecular size, but not as quickly as expected by simple RRK theory. This behavior along with temperature dependence studies suggests that the internal energy required for dissociation is provided in substantial part by both the initial thermal internal energy and the energy imparted by the photoionization step. The role of thermal energy in the dissociation of large ions is discussed.     

Infrared multiphoton dissociation of CHFCl2

We have studied the dependence of the IR laser induced multiphoton dissociation of CHFCl₂ on laser wavelength and fluence, number of laser pulses and initial CHFCl₂ pressure. Multiphoton dissociation spectrum presents a broad maximum centered at 9.342 μm. Dissociation has a strongly dependence on initial CHFCl₂ pressure and laser fluence. There exists a pressure lower limit (≈ 0.4 mb) below which no significant dissociation occurs. Up to 2.1 J/cm² no unimolecular dissociation takes place in a significant proportion. The only radical we have been able to clearly detect by real time optical absorption technique is CFCl. This supports the mechanism reaction CHFCl₂ + nhν → CFCl + HCl.     

Spectrophotometric determination of copper with α, β, γ, δ-tetraphenylporphine trisulfonate

Water-soluble porphyrin, α, β, γ, δ-tetraphenylphorphine trisulfonate (TPPS, H₂R), was found to be a very useful agent for both the direct spectrophotometric determination and the photometric titration of copper(II). The molar absorptivity of H₄R²⁺ at 434 nm is 5.0·10⁵ and the spectrophotometric sensitivity is 0.00013 μg Cu cm^?2 for A=0.001. Beer's law is followed in the range 0.006 μg–0.06 μg Cu ml^?1. Among twenty-two elements examined, only zinc(II) seriously interfered. Acid dissociation constants and salt effects on the spectra of TPPS were evaluated.     

Reactor neutrons irradiation effect on the photocatalytic activity of SnO<Subscript>2</Subscript> thin films

SnO₂ thin films synthesized by sol-gel are irradiated with reactor neutrons up to fast neutron fluence of 9.6 × 10¹⁷ neutrons cm^–2 at 40°C. The influence of defects generated by neutrons irradiation, through the properties modification, on the photo-catalytic activity of SnO₂ films is investigated. It is found that the photoactivity of the irradiated films is enhanced after reactor neutrons irradiation. An improvement of 41% is observed for the sample irradiated at a neutron fluence of 9.6 × 10¹⁷ neutrons cm^–2. This is attributed to several parameters modified by the reactor neutron irradiation principally the crystallite size and space charge region which are closely related to the photocatalytic performance.     

Solid-state study of hydrazonium tartrate and deuterated hydrazonium tartrate enantiomers

A study of the crystallographic, optical, and thermochemical properties of hydrazonium tartrate and deuterated hydrazonium tartrate enantiomers is described. Crystals of the enantiomers are orthorhombic with a tetramolecular cell. The space group is P2₁2₁2₁ with the lattice parameters a₀ = 7.640 ± 0.002 Å, b₀ = 13.441 ± 0.003 Å, and c₀ = 7.029 ± 0.002 Å. No change in lattice parameters is observed on deuteration. Optical second harmonic powder analysis shows the crystals to be phase matchable at 1.06 μm with d^2ω = 11 d^2ωα-SiO₂. The optical nonlinearity being unaffected by deuterium substitution is attributed to the nonlinear electronic polarizability of the hydrogen bonds. Crystals are transparent from 239 nm to 1.61 μm. Deuteration shifts the long wavelength cutoff to 2.07 μm, without affecting the band edge.     

Concentration dependence of the relative error in diffuse reflectance infrared spectrometry

A mathematical model between the relative error in the Kubelka—Munk (K—M) function and the sample concentration has been determined if the K—M function is linear with the sample concentration, c≤ w/w%. The theoretical model has been investigated by measuring 3–5 parallels at different sample concentrations and calculating the RSD for the selected absorption bands. Quartz (d_ave = 1.3 μm) and calcite (d_ave = 3.3 μm) as analytes and KBr (d_ave = 9.9 μm) as embedding material were used. The result of the model and the experiments were in a good agreement. It has been shown that the RSD for absorption bands with small sensitivity can increase up to ±20–60%. The precision of the quantitative analysis in diffuse reflectance infrared Fourier transform spectrometry (DRIFTS) can be improved by applying more sensitive absorption bands and parallel measurements at one standard concentration     

Ionization-induced nucleation above liquid beam of aqueous solution of phenol after IR laser irradiation

A continuous liquid flow of an aqueous solution of phenol (Ph) in a vacuum (a liquid beam) was irradiated with a pulsed IR laser at 3 μm, which was resonant to the OH-stretching vibration of the solvent water molecules. Phenol molecules ejected from the liquid beam were selectively ionized at about 0.5 mm above it by a pulsed UV laser (270–280 nm). The photoions thus produced were extracted in a pulsed electric field with a given residence time after the photoionization for mass analysis. It was shown that photoions, Ph⁺, were solvated into Ph⁺(H₂O)_n in a dense cloud of water vapor ejected from the liquid beam by IR irradiation.     

A new class of azobenzene chelators for Mg and Ca in buffer at physiological pH

A new class of azobenzene-based chelators, trans-3a and trans-3b (3a and 3b), were designed and synthesized in two steps. Both 3a and 3b were readily dissolved in a buffer solution at physiological pH. The values of the dissociation constant of 3a and 3b for Mg²⁺ and Ca²⁺ were determined by the Hills plot; K_d^Mg=1.12 mM and K_d^Ca=660 μM for 3a and K_d^Mg=158 μM and K_d^Ca=200 μM for 3b, respectively. On irradiation at 489 nm light, 3a isomerized to give cis-form, which underwent cis-to-trans thermal isomerization in darkness at room temperature. The change in the absorption spectrum of the irradiated solution of 3a in the presence of Mg²⁺, showing the cis-to-trans thermal isomerization, indicates that the affinity of cis-3a for Mg²⁺ is lower than that of 3a.     

Effect of droplet size on the phosphine depression of calcium atomic emission signals in flame spectrometry

The effect of the droplet size on the magnitude of the phosphine depression of calcium signals is discussed. The droplet size governs the time required for droplet desolvation in the flame. It is during the desolvation process that the combustion products of phosphine, PO_x, diffuse into the droplet and form a refractory compound with the analyte. The longer the desolvating droplet resides in the PO_x-contaminated flame, the more severe the depression. A uniform droplet generator, a pneumatic nebulizer spray chamber system, and a glass-frit nebulizer spray chamber system were the sample introduction systems studied. Droplet sizes of (55 μm, 0.5–10 μm (2 μm mean), and <0.1–2 μm (0.1 μm mean) were produced by these systems, respectively, and depressions of the calcium signals of 57%, 55%, and 4% were noted. These results suggest that the phosphine depression on calcium signals may be alleviated by using a glass-frit nebulizer (or modifying a commercial nebulizer) to remove droplets greater than 2 μm in diameter.     

A study of some problems in determining the stoicheiometric proton dissociation constants of complexes by potentiometric titrations using a glass electrode

Possible errors in the measurement of acid dissociation constants by potentiometric titration techniques have been considered, with particular references to nitrilotriacetic acid (NTA) and ethylenediaminetetraacetic acid (EDTA). Unknown junction potentials can arise when pH measurements are carried out using a glass electrode with saturated calomel reference electrode which have been previously calibrated with a standard buffer solution. The magnitude of the influence of these unknown potentials has been demonstrated and an experimental procedure recommended which gives meaningful results.The precision of calculated acid dissociation constants will also be influenced by the presence of cationic species (e.g. H₄L⁴), the total acid strength, the absolute values of the constants and the value accepted for the auto-dissociation constant of water (K_w). All these factors have been considered quantitatively and their effect on metal complex formation constants, calculated from these acid dissociation constants, noted. The proton dissociation constant of the cationic species of NTA (i.e. H₄L⁺) has been found to have the value of pK₀=0.80 at 20° and μ=0.10 M.     

Synthesis,in silico and in vitro Evaluation of Novel Oxazolopyrimidines as Promising Anticancer Agents

New potential bioactive oxazolopyrimidines have been synthesized using two main approaches: the pyrimidine ring annulation on a functionalized oxazole and the benzoyl bromide trimerization followed by rearrangement and formation of the oxazolo[5,4-d]pyrimidine scaffold. The docking analyzes have shown that 7-piperazine substituted oxazolo[4,5-d]pyrimidines 8a – 8c could be potential VEGFR2 inhibitors with high free energy of ligand–protein complex formation (ΔG: −10.1, −9.6, −9.8 kcal/mol, respectively). In vitro antitumor assays confirmed theoretical predictions that oxazolo[4,5-d]pyrimidines 8a – 8c containing positively charged piperazine moiety should demonstrate significantly higher cytotoxic effects. 4-[5-(4-Chlorophenyl)-2-phenyl[1,3]oxazolo[4,5-d]pyrimidin-7-yl]piperazin-1-ium trifluoroacetate ( 8c ) exhibited a slightly higher antiproliferative effect (IC₅₀=0.21 μm ) than doxorubicin (IC₅₀=0.36 μm ) on MDA-MB-231 cell line and has relatively good results on OVCAR-3 (IC₅₀=1.7 μm ) and HCT-116 (IC₅₀=0.24 μm ) cells.     

Long-range interactions in molecules and rotational coupling

We report a case study on Na₂ of the influence of rotational coupling for molecular states directly below the dissociation limit, where the electronic binding energy and the hyperfine interactions are of similar magnitude and the rotational energy can be varied from small to large compared to the former energies. The experimental observation and the theoretical analysis are important for obtaining precise data concerning long-range interactions and extrapolation to the dissociation limit, which are required for describing cold collisions in atomic traps. A consistent model for all observations with rotational quantum number J′ up to 41 is developed which involves few atomic parameters and demonstrates that these are sufficient to describe molecular levels few μeV below the dissociation energy.