Relative rate constants for removal of vibrationally excited OH(X2πi)v=9 by some small molecules at room temperature

Vibrationally excited OH in v = 9 [designated OH^?(9)] was generated by the reaction of hydrogen atoms with ozone in a fast-flow discharge system at 300 ± 3 K and a total pressure of 1.1 ± 0.1 torr, with argon as the carrier gas. The addition of a species X, which can deactivate the OH^?(9) or react with it, led to a decrease in the Meinel band chemiluminescent emission intensities at both 626 nm (9 → 3 band) and 519 nm (9 → 2 band), which were monitored as a function of the concentration of X. Application of the kinetic scheme developed previously for this chemical system gave the relative rate constant for the removal of OH^?(9) by X. The relative rate constants determined in this study, taking O₂ as the reference deactivator (k = 1.0), are as follows: He ≤ 0.02; H₂ ≤ 0.05; SF₆ 0.09 ± 0.01; CF₄ 0.19 ± 0.01; N₂O 3.5 ± 0.4; NO 17.7 ± 1.5; H₂O 74.3 ± 2.9; D₂O 57.6 ± 2.0; NH₃ 61.3 ± 1.9; ND₃ 58.7 ± 1.6; SO₂ 7.1 ± 1.4; COS 8.4 ± 1.7; H₂S 33.7 ± 8.4; CH₄ 1.56 ± 0.03; CD₄ 1.06 ± 0.06. Application of these relative rate constants to conditions in the upper atmosphere (60–100 km) suggests that OH^?(9) is removed primarily by deactivation by O₂, and at altitudes ?90 km, possibly by O(³P). However, since O₂ is unusually efficient for a homonuclear diatomic in deactivating OH^?(9), it may not be the primary deactivator for the lower (v ≤ 8) vibrational levels. These results are compared to earlier studies of OH^?(9), and possible mechanisms of interaction of OH^?(9) with these molecules are discussed.     

Deactivation of vibrationally excited hydrogen fluoride (v=2 and v=1) by atomic fluorine

Measurements have been made which provide information concerning the rate of energy transfer between vibrationally excited HF and atomic fluorine. It was found that HF (v = 1) deactivates about seven times slower than was determined in previous experiments. The deactivation rate constant for HF (v = 2) is about six times larger than for HF (v = 1).     

Experimental measurement of the rate of the reaction o(3P) + H2(v = 0) → OH(v = 0) + H at T = 298 K

Measurement of the rate of the reaction is reported. The measurements were made in a flow tube apparatus. The result is based on data for the absolute density of OH(v = 0) obtained from laser-induced fluorescence measurements in the (0–0) band of the OH(A²Σ⁺ → X²II) system. The density of oxygen atoms was varied by changing the flow rate of NO which is consumed in the reaction N + NO → O + N₂. We find that k₁ (298 K) = (5.5 ± 3.0) × 10⁶ cm³/mol sec. This result was obtained with consideration and control of the effect of reaction (2): for which vibrationally excited hydrogen is created by energy transfer in the presence of active nitrogen. It was found that the addition of N₂ or CO₂ effectively suppressed the excitation of H₂(v = 1). Measurements of the density of H₂(v = 1) were made by VUV absorption in the Lyman band system of H₂. All of the reports of low-temperature measurements and some recent theoretical calculations for k₁ are discussed. The present result confirms and extends the growingevidence for significant curvature in the low-temperature end of a modified Arrhenius plot of k₁ (T).     

The OH(v = 9) + O3 reaction pathway

The oxygen-hydrogen system, including the reactive species H, O, H₂, O₂, O₃, OH, and HO₂, is very complex, and contains numerous reactions whose kinetics and branches have been insufficiently explored. In the present study we use computer modeling to simulate observations made in a 300-K ozone-hydrogen mixture, in which a critical H₂ pressure leads to rapid ozone decomposition, and generation of high concentrations of atomic oxygen. Initiation of the reaction chain involves heterogeneous O and/or H atom production, and the chain branching step is the reaction OH(v) + O₃ → OH + O + O₂, which is shown to be the predominant pathway for these reactants. The critical H₂ pressure (ca. 3 torr) sets important constraints upon the system kinetics.     

Kinetics of CN(v=0) and CN(v=1) with H2 HCl and HBr

CN radicals have been generated in their X ²Σ⁺ (v=0) and (v= 1 ) levels by pulsed laser photolysis of NCNO at 532 nm, and time-resolved laser-induced fluorescence has been used to measure the rates of their removal by H₂, HC1 and HBr. The rate constants for removal of CN(v= 1 ) by these three species are 1.2 ± 0.3, 1.1 ± 0.2 and 1.3 ± 0.1 times the rate constants for reaction of CN(v=0). The results can be interpreted in terms of vibrationally adiabatic theory and a CN vibrational frequency which is almost the same in the transition state as in the isolated radical.     

[Pb2(AMP)2(μ‐X)2X2], X = Br− and I−, AMP = 2‐aminomethylpyridine,Two New Dimeric Lead(II) Complexes Extended in One‐dimensional Helical Chain Polymers by Noncovalent π–π‐stacking

The two lead(II) complexes [Pb₂(AMP)₂(μ‐X)₂X₂], X = Br^?, I^? and AMP = 2‐aminomethylpyridine, have been synthesized and characterized. Self‐assembly of these compounds in the solid state via π–π‐stacking interactions is discussed.     

Rotationally inelastic scattering of OH (2Pi 3/2, v=0, J=3/2, f) by HBr (1Sigma, v=0, J<4)

Relative state-to-state cross sections of OH molecules in the (2)Pi(32), v=0, J=32, M(J)=32, f state have been determined for transitions up to (2)Pi(32), v=0, J=112, f and (2)Pi(12), v=0, J=72, e states by collisions with HBr molecules ((1)Sigma, v=0, J<4) at 750 cm(-1) collision energy. In order to investigate features of the anisotropy of the OH-HBr potential energy surface, the steric asymmetries, which account for the effect of the OH orientation with respect to the collision partner, have been measured. A comparison with other systems previously studied shows strong similarities with the OH-HCl system.     

State-resolved collisional quenching of vibrationally excited pyrazine (E(vib) = 37,900 cm(-1)) by D35Cl(v = 0)

Supercollision relaxation of highly vibrationally excited pyrazine (E(vib) = 37,900 cm(-1)) with D35Cl is investigated using high-resolution transient IR diode laser absorption spectroscopy at 4.4 microm. Highly excited pyrazine is prepared by pulsed UV excitation at 266 nm, followed by rapid radiationless decay to the ground electronic state. The rotational energy distribution of the scattered DCl (v = 0,J) molecules with J = 15-21 is characterized by T(rot) = 755+/-90 K. The relative translational energy increases as a function of rotational quantum number for DCl with T(rel) = 710+/-190 K for J = 15 and T(rel) = 1270+/-240 K for J = 21. The average change in recoil velocity correlates with the change in rotational angular momentum quantum number and highlights the role of angular momentum in energy gain partitioning. The integrated energy-transfer rate for appearance of DCl (v = 0,J = 15-21) is k(2)(int) = 7.1x10(-11) cm3 molecule(-1) s(-1), approximately one-eighth the Lennard-Jones collision rate. The results are compared to earlier energy gain measurements of CO2 and H2O.     

C—H...X (X = O,N or π) interactions in benzyl carbamate

The crystal packing and interaction energy of benzyl carbamate, C₈H₉NO₂, have been analysed in detail by the PIXEL method. Benzyl carbamate forms layers of hydrogen‐bonded molecules, with the layers connected by weaker C—H...π interactions. According to the PIXEL analysis, combinations of C—H...X (X = O, N or π) interactions are comparable in energy with hydrogen bonding. These interactions are necessary for explaining the geometry and the assembly of the layers.     

Quantum state-to-state dynamics for the quenching process of Br(2P1/2) + H2(v(i) = 0, 1, j(i) = 0)

Quantum state-to-state dynamics for the quenching process Br((2)P(1/2)) + H(2)(v(i) = 0, 1, j(i) = 0) → Br((2)P(3/2)) + H(2)(v(f), j(f)) has been studied based on two-state model on the recent coupled potential energy surfaces. It was found that the quenching probabilities have some oscillatory structures due to the interference of reflected flux in the Br((2)P(1/2)) + H(2) and Br((2)P(3/2)) + H(2) channels by repulsive potential in the near-resonant electronic-to-vibrational energy transfer process. The final vibrational state resolved integral cross sections were found to be dominated by the quenching process Br((2)P(1/2)) + H(2)(v) → Br((2)P(3/2)) + H(2)(v+1) and the nonadiabatic reaction probabilities for Br((2)P(1/2)) + H(2)(v = 0, 1, j(i) = 0) are quite small, which are consistent with previous theoretical and experimental results. Our calculated total quenching rate constant for Br((2)P(1/2)) + H(2)(v(i) = 0, j(i) = 0) at room temperature is in good agreement with the available experimental data.     

Crystallographic and Spectroscopic Evidence for an Intramolecular (OH … π)-Interaction

Crystallographic and spectroscopic evidence for an intramolecular (OH … π)-interaction in anti^9,10-10endo-hydroxy, 10exo-butyltricyclo [4.2.1.1^2.5]deca-3, 7-dien-9-one ( 1 ) is presented.     

Photodetachment microscopy of the P, Q, and R branches of the OH(-)(v=0) to OH(v=0) detachment threshold

A photodetachment experiment is performed on the v=0-->v=0 OH(-) detachment threshold. The weak O and S branches provide a signal strong enough to make amplitude measurements on all five O, P, Q, R, and S branches possible, which are used to fix the formulas for their relative intensities. Photodetachment microscopy is applied to 15 different thresholds of the P, Q, and R branches. The quantitative analysis of the interference patterns obtained does not show any effect of the dipole moment of OH, but yields a new measurement of the rotational parameters of OH(-)(v=0) and of the electron affinity of the molecule. The new recommended value for the electron affinity of (16)O(1)H is 14 740.982(7) cm(-1) or 1.827 648 7(11) eV.     

Halogenverbrückte Heterometallatomcluster der drei Typen Re2(CO)4L2(μ-X)2(μ-Y) (L = (C6H5)3P; X = Br,I; Y = GaRe(CO)4ax-L), Re2(CO)6L2(μ-X)(μ-GaX2) (X = I) und Re3(CO)9L3(μ-X)3(μ-Y) (X = Cl)

Halogeno-Bridged Heteronuclear Metal Atom Clusters of the Three Types Re₂(CO)₄L₂(μ-X)₂(μ-Y) (L = (C₆H₅)₃P; X = Br, I; Y = GaRe(CO)₄ax-L), Re₂(CO)₆L₂(μ-X) (μ-GaX₂) (X = I), and Re₃(CO)₉L₃ (μ-X)₃(μ₃-Y) (X = Cl) The title compounds of the both types Re₂(CO)₄L(μ-X)₂(μ-Y) [L = (C₆H₅)₃P; X = Br, I; Y = GaRe(CO)₄ax-L] and Re₃(CO)₉L₃(μ-X)₃ (μ₃-Y) (X = Cl) were prepared by the reaction of GaX₃ (X = Cl, Br, I) and Re₂(CO)₈(ax-L)₂ in boiling mesitylene solution. The obtained substance Re₂(CO)₄L₂(μ-I)₂(μ-Y) and carbon monoxide gave the compound of the third type Re₂(CO)₆L₂(μ-I)(μ- GaI₂). The last-named single iodo-bridged dirhenium cluster could be therefore a precursor complex of the double iodo-bridged compound. The four diamagnetic substances were characterized by ³¹P n.m.r. spectroscopy and their molecular structures were acertained by X-ray measurements. The result of the single crystal X-ray analysis of Re₂(CO)₄L₂(μ-Br)₂ [μ-GaRe(CO)₄ax-L], a bridged coordination octahedron pair with a common face, and that of the edge-bridged pair Re₂(CO)₆L₂(μ-I)(μ-GaI₂) each possessing a Re? Re bond are especially treated in the present work.     

Copper(0)‐mediated living radical polymerization of acrylonitrile at room temperature

The copper(0)‐catalyzed living radical polymerization of acrylonitrile (AN) was investigated using ethyl 2‐bromoisobutyrate as an initiator and 2,2′‐bipyridine as a ligand. The polymerization proceeded smoothly in dimethyl sulphoxide with higher than 90% conversion in 13 h at 25 °C. The polymerization kept the features of controlled radical polymerization. ¹H NMR spectra proved that the resultant polymer was end‐capped by ethyl 2‐bromoisobutyrate species. Such polymerization technique was also successfully introduced to conduct the copolymerization of styrene (St) and AN to obtain well‐controlled copolymers of St and AN at 25 °C, in which the monomer conversion of St could reach to higher than 90%. © 2010 Wiley Periodicals, Inc. J Polym Sci Part A: Polym Chem, 2011     

Vibrational relaxation of O2(X3 Sigma g-, v = 9-13) by collisions with O2

Vibrationally excited O(2)(X(3) Sigmag(-)) was generated in the UV laser flash photolysis of O(3) and single vibrational level was detected via laser-induced fluorescence (LIF) in the B(3) Sigmau(-)-X(3) Sigmag(-) system. The time-resolved LIF of adjacent vibrational levels has been analyzed by the integrated-profiles method and the rate coefficients for single-quantum relaxation, O(2)(X(3)Sigmag(-), v = 9-13)+ O(2)(v = 0)--> O(2)(X(3)Sigmag(-), v - 1)+ O(2)(v = 1), have been determined. To the best of our knowledge, the rate coefficients for v = 12 and 13 are measured for the first time in the present study. The efficiency of relaxation is higher at lower vibrational levels, indicating that a small energy mismatch is suitable for the energy transfer. The vibrational level dependence of all the rate coefficients for the relaxation measured in the present study and previously reported by several groups can be rationalized by the energy gap law.