Laser photodissociation of s-tetrazine: Product vibrational excitation

The photosensitive and thermally unstable molecule s-tetrazine decomposes to yield one nitrogen molecule and two HCN molecules. Following pulsed irradiation of tetrazine vapor at 492.3 nm, we have observed time resolved infrared fluorescence from HCN(001). In a similar experiment, small quantities of CO₂ were added to the sample cell, and we observed infrared fluorescence from CO₂ (001) populated by VV energy transfer. From fluorescence intensity measurements, we have been able to estimate the amount of excitation in certain product vibrations. We conclude that ≈ 1% of the HCN is produced in the (001) state, and the “equivalent” of ≈ 0.1 quantum of N₂ vibrational excitation is excited. This latter figure may include some excitation of HCN (ν₁), but the measured energy transfer rate coefficients are consistent with N₂ excitation. The small amount of HCN(ν₃) and N₂ vibrational excitation is surprising, as the photodissociation is exothermic by more than 100kcal/mole.     

活性氮与碘乙烷反应化学发光研究

在流动余辉装置上, 利用N₂空心阴极放电制备活性氮, 研究了活性氮与碘乙烷(C₂H₅I)反应的化学发光. 在620～820 nm波长范围内观察到了较强的发射光谱, 拟合得到的光谱常数表明它来源于NI(b¹Σ^＋→X³Σ^－)跃迁, 并对35个谱峰进行了振动归属. 最后讨论了活性氮中主要成分与C₂H₅I反应的可能过程, 结合辅助性实验分析表明, 活性氮中的N(²P)与C₂H₅I直接反应很可能产生激发态NI(b¹Σ^＋)自由基. 这是利用化学反应直接产生激发态NI(b¹Σ^＋)的首次报道, 观察到的激发态最高振动能级为v'＝6.     

Plasma diagnostics of barrier-torch discharge in argon flow in a capillary by cross-correlation spectroscopy

The radiation kinetics of the plasma of barrier-torch disrcharge in argon flow in a capillary has been studied by cross-correlation spectroscopy. It was established that the discharge emission spectrum consists of peaks of electronically excited states of argon, bands of hydroxyl radicals, and a second positive system of nitrogen. An analysis of the spatio-temporal distributions of emission intensity for the selected spectral indicators showed that the causes of the torch are ionization waves that extend through the capillary from the electrode system with a speed of 10⁵ m/s and project up to 3–4 mm. It was established that the formation of electronically excited molecules of nitrogen N₂(C ³Π _u ) in the torch of discharge occurs mainly on the reaction between metastable electronically excited atoms of argon and molecules of nitrogen in the electronic ground state.     

The reactions of atomic hydrogen and active nitrogen with hydrogen azide

Detection of atoms by mass spectrometry has been used to study the reactions of hydrogen azide, HN₃, with H atoms and active nitrogen, in a fast flow reactor at pressures of about 1 torr. Stoichiometry and products of the H + HN₃ reaction have been determined and the rate constant of the initial step, assumed to be H + HN₃ → NH₂ + N₂, was found to be 2.54 × 10^?11 exp (?4600/RT) cm³ molecule^?1 s^?1, in the temperature range of 300–460K. The formation of NH₃ and H₂ products has been discussed from the different secondary steps which may occur in the mechanism. For the reaction of active nitrogen with HN₃, evidence has been found for the participation of excited nitrogen molecules produced by a microwave discharge through molecular nitrogen. The influence of excited nitrogen molecules has been reduced by lowering the gas flow velocity. It was then possible to study the N + HN₃ reaction for which the rate constant of the initial step was found to be 4.9 × 10^?15 cm³ molecule^?1 s^?1 at room temperature. Finally, the occurrence of these elementary reactions has been discussed in the mechanism of the decomposition flame of HN₃.     

He-N2 radiofrequency discharge: Influence of N2 on discharge and afterglow

A diagnostic study q (energy transfer processes in a He-N₂ flowing discharge and afterglow has been performed in a radiofrequency-produced plasma cooled in a liquid nitrogen hath. Optical emission spectroscopy in the visible and infrared spectral range as well as Langrnuir probe diagnostics were used. The vibrational kinetics of CO injected in such an afterglow has been examined. It shows a slow cooling of the electrons in the afterglow regime. The electron kinetics responsible joy CO vibrahonal excitation is turned off when N₂ is added to the He discharge, while that for vibrationally excited N₂ molecules is turned on. The results are discussed on the basis of previous theorerical calculations and experiments on the He-N₂ system.     

Initial state selection and intramolecular vibrational relaxation in reacting polyatomic molecules. Isopropylcyclobutane precursor

The study of intramolecular vibrational energy transfer in polyatomic molecules excited to the level of chemical reaction is here extended to hydrocarbon species. By insertion of ¹CH₂ into the CH bonds of isopropylcyclobutane a closely related series of chemically activated alkyl cyclobutanes are produced at levels of excitation above 100 kcal mole^?1. The cyclobutane ring decomposes into olefin fragments. The methylene insertion takes place at CH sites on the molecule which are either on the ring or on the side chain. This corresponds to injection of excited molecules into various regions of their energy-coordinate hyperspace which are more or less adjacent to, or remote from the critical hyperplane corresponding to decomposition. A study of the pressure dependence of the relative rates and amounts of decomposition of the several differentially excited cyclobutanes follows theoretical expectations with regard to occurrence of non-randomized decomposition from some of the molecules prior to complete relaxation. Molecules which have been activated on the side chain exhibit only ordinary randomized decomposition. Analysis of the data on a simple model leads to gross rates of intramolecular relaxation, λ = 2.2 × 10¹²s^?1 and λ = 3.5 × 10¹²s^?1, for species excited at different sites on the ring. These rates are several times larger than those previously reported for fluorocyclopropanes.     

Calculation of some nitrogen nuclear screening constants

Some nitrogen screening constants and their anisotropies are calculated within the CNDO/S level of approximation. Satisfactory agreement is found with available experimental data in most cases. In general the reported results are in closer agreement with experiment than are those found from ab initio calculations. The calculated data for the isoelectronic molecules N₂O and CH₂N₂ would be in better agreement with experiment if the assignments of the two nitrogen nuclei were reversed in both cases. A reasonable correlation is obtained with some observed nitrogen chemical shifts. Contributions arising from electronic transitions are reported for N₂, HCN, CH₃CN, CH₃NC, NO₂⁺ and NO₂^?.     

Reactions of Adsorbed CH3 Radicals and the Products of Their Decomposition at Mo and Cu Surfaces According to Spatially Resolved TPR Data

Reactions in the layer of CH₃ radicals adsorbed on the surfaces of polycrystalline molybdenum and copper were studied using the method of temperature-programmed reaction (TPR). After N₂ and CH₃ ^· adsorption (the products of azomethane pyrolysis) on molybdenum, N₂, H₂, and CH₄ were observed in comparable amounts in the TPR spectrum. At the same time, only methane was detected in the TPR products on the copper surface. The spatial distributions of CH₄ desorption flows were measured, which were indicative of translational excitation of these molecules. The direct measurements of the rates of the CH₄ molecules desorbed from the copper surface showed that their translational energy was 10–15 times greater than the thermal one. The mechanisms of reactions on the Mo and Cu surfaces are proposed. The rate constants were calculated for some of the elementary steps.     

Effect of excitation states of nitrogen on the surface nitridation of iron and steel in d.c. glow discharge plasma

The plasma nitriding phenomena that occur on the surfaces of iron and steel were investigated. In particular, the correlation between the kinds of nitrogen radicals and the surface nitriding reaction was investigated using a glow‐discharge apparatus. To control the excitation of nitrogen radicals, noble gas mixtures were used for the plasma gas. The highly populated metastables of noble gases selectively produce excited nitrogen molecules (N₂*) or nitrogen molecule ions (N₂⁺). The optical emission spectra suggested that the formation of N₂*‐rich or N₂⁺‐rich plasma was successfully controlled by introducing different kinds of noble gases. Auger electron spectroscopy and XPS were used to characterize the depth profile of the elements and chemical species on the nitrided surface. The nitride layer formed by a N₂⁺‐rich plasma had a much higher nitrogen concentration than that by a N₂*‐rich plasma, likely due to the larger chemical activity of the N₂⁺ species as well as the N₂⁺ sputtering bombardment to the cathode surface. The strong reactivity of the N₂⁺ species was also confirmed from the chemical shift of N 1s spectra for iron nitrides. An iron nitride formed by the N₂⁺‐rich plasma has higher stoichiometric quantity of nitrogen than that formed by the N₂*‐rich plasma. Besides the effect of nitrogen radicals on surface nitridation, the contribution of the chromium in steel to the nitriding reaction was also examined. This chromium can promote a nitriding reaction at the surface, which results in an increase in the nitrogen concentration and the formation of nitride with high nitrogen coordination. Copyright © 2010 John Wiley & Sons, Ltd.     

Contribution of Discharge Excited Atomic N,N2*, and N2+ to a Plasma/Liquid Interfacial Reaction as Suggested by Quantitative Analysis

Electric-discharge nitrogen comprises three main types of excited nitrogen species-atomic nitrogen (N_atom), excited nitrogen molecules (N₂*), and nitrogen ions (N₂⁺) – which have different lifetimes and reactivities. In particular, the interfacial reaction locus between the discharged nitrogen and the water phase produces nitrogen compounds such as ammonia and nitrate ions (denoted as N-compounds generically); this is referred to as the plasma/liquid interfacial (P/L) reaction. The N_atom amount was analyzed quantitatively to clarify the contribution of N_atom to the P/L reaction. We focused on the quantitative relationship between N_atom and the produced N-compounds, and found that both N₂* and N₂⁺, which are active species other than N_atom, contributed to P/L reaction. The production of N-compounds from N₂* and N₂⁺ was enhanced upon UV irradiation of the water phase, but the production of N-compounds from N_atom did not increase by UV irradiation. These results revealed that the P/L reactions starting from N_atom and those starting from N₂^* and N₂⁺ follow different mechanisms.     

CN chemiluminescence in N2 + CH4 Flowing afterglow at low temperatures

The spectra of flowing microwave post-discharge excited in N₂ and N₂ + CH₄(N₂ + C₂H₂) gas mixtures have been studied at low temperature (77 K). The molecular spectra of CN emitted by the collision-induced N + C and N + CH chemiluminescent reactions in the low-temperature afterglow system have been thoroughly investigated. The intensity of different CN (B²⁺-X²⁺) vibrational bands is very sensitive to low hydrocarbon concentration in nitrogen used as the working gas. Detection of hydrocarbon species has been demonstrated from concentrations of CH₄ and C₂H₂ in N₂ greater than 10¹⁰ molecules · cm^–3.     

CARS Diagnostic and Modeling of a Dielectric Barrier Discharge

Dielectric barrier discharges (DBD) with planar- and knife-shaped electrodes are operated in N₂O₂NO mixtures under a pressure of 20 and 98 kPa. They are excited by means of consecutive unipolar or bipolar high-voltage pulse packages of 10 kV at a pulse repetition rate of 1 and 2 kHz. The rotational and vibrational excitation of N ₂ molecules and the reduction of nitric oxide (NO) in the discharge have been investigated using coherent anti-Stokes Raman scattering (CARS) technique. Rotational (gas) temperatures near the room temperature and vibrational temperatures of about 800 K at atmospheric pressure and 1400 K at a pressure of 20 kPa are observed. Therefore, chemical reactions of NO with vibrationally excited N ₂ are probably insignificant. One-dimensional kinetic models are developed that balance 35 chemical reactions between 10 species and deliver equations for the population density of excited vibrational levels of N ₂ together with a solution of the Boltzmann equation for the electrons. A good agreement between measured vibrational temperatures of N ₂ , the concentration of NO, and calculated data is achieved. Modeling of the plasma discharge verifies that a DBD operated with a N₂NO mixture reduces the NO content, the simultaneous presence of O ₂ , already 1%, is enough to prevent the NO reduction.     

Kinetics and mechanism of the reaction of Cl atoms with CH2 CO (Ketene)

The kinetics and mechanism of the gas-phase reaction of Cl atoms with CH₂CO have been studied with a FTIR spectrometer/smog chamber apparatus. Using relative rate methods the rate of reaction of Cl atoms with ketene was found to be independent of total pressure over the range 1–700 torr of air diluent with a rate constant of (2.7 ± 0.5) × 10⁻¹⁰ cm³ molecule⁻¹ s⁻¹ at 295 K. The reaction proceeds via an addition mechanism to give a chloroacetyl radical (CH₂ClCO) which has a high degree of internal excitation and undergoes rapid unimolecular decomposition to give a CH₂Cl radical and CO. Chloroacetyl radicals were also produced by the reaction of Cl atoms with CH₂ClCHO; no decomposition was observed in this case. The rates of addition reactions are usually pressure dependent with the rate increasing with pressure reflecting increased collisional stabilization of the adduct. The absence of such behavior in the reaction of Cl atoms with CH₂CO combined with the fact that the reaction rate is close to the gas kinetic limit is attributed to preferential decomposition of excited CH₂ClCO radicals to CH₂Cl radicals and CO as products as opposed to decomposition to reform the reactants. As part of this work ab initio quantum mechanical calculations (MP2/6-31G(d,p)) were used to derive Δ_fH₂₉₈(CH₂ClCO) = −(5.4 ± 4.0) kcal mol⁻¹. © 1996 John Wiley & Sons, Inc.     

Energy partitioning and reaction dynamics in the chemiluminescent channel of the reaction: HS + O3 → HSO* + O2

The title reaction forms electronically excited HSO(òA′) directly, with considerable vibrational and rotational excitation as well. The internal excitation of the HSO fragment is the maximum possible consistent with the concurrent formation of an O₂(¹Δ_g) molecule as the other reaction product. The observed vibrational excitation peaks in the υ′= 2 level of the υ₃ mode. No evidence about possible excitation of the other vibrational modes of HSO could be obtained.     

Catalytic decomposition of azomethane and reactions of adsorbed methyl radicals on the molybdenum surface

The methods of temperature-programmed reaction/desorption (TPR/TPD) are used to study azomethane (CH³N=NCH³) decomposition and the reactions of the products of its pyrolysis (CH ₃ ^* radicals and N₂) on the polycrystalline molybdenum surface. A TPR spectrum of adsorbed azomethane decomposition shows mainly N₂, H₂, and unreacted azomethane. Upon preliminary adsorption of azomethane pyrolysis products on a catalyst sample, a TPR spectrum shows N₂, H₂, and CH₄ in comparable amounts. The difference in the composition of desorption products found for these two types of experiments shows that, in the decomposition of adsorbed azomethane, surface methyl moieties are not formed. The rate constants were calculated for the dissociation of adsorbed CH₃, CH₂, and CH, recombination of hydrogen atoms with each other and with CH₃ and CH₂, and the recombinative desorption of nitrogen atoms. Deceased.     

Discriminating alkylbenzene isomers with tandem mass spectrometry using a dielectric barrier discharge ionization source

Soft ambient ionization sources generate reactive species that interact with analyte molecules to form intact molecular ions, which allows rapid, sensitive, and direct identification of the molecular mass. We used a dielectric barrier discharge ionization (DBDI) source with nitrogen at atmospheric pressure to detect alkylated aromatic hydrocarbon isomers (C₈H₁₀ or C₉H₁₂). Intact molecular ions [M]^•+ were detected at 2.4 kV_pp, but at increased voltage (3.4 kV_pp), [M + N]⁺ ions were formed, which could be used to differentiate regioisomers by collision-induced dissociation (CID). At 2.4 kV_pp, alkylbenzene isomers with different alkyl-substituents could be identified by additional product ions: ethylbenzene and -toluene formed [M-2H]⁺, isopropylbenzene formed abundant [M-H]⁺, and propylbenzene formed abundant C₇H₇⁺. At an operating voltage of 3.4 kV_pp, fragmentation of [M + N]⁺ by CID led to neutral loss of HCN and CH₃CN, which corresponded to steric hindrance for excited state N-atoms approaching the aromatic ring (C-H). The ratio of HCN to CH₃N loss (interday relative standard deviation [RSD] < 20%) was distinct for ethylbenzene and ethyltoluene isomers. The greater the number of alkyl-substituents (C-CH₃) and the more sterically hindered (meta > para > ortho) the aromatic core, the greater the loss of CH₃CN relative to HCN was.     

Determination of C-atom density downstream an Ar-CH4 rf plasma torch

Nitrogen, oxygen, and carbon atoms have been detected by optical emission spectroscopy in a common flowing post-discharge of an Ar-x CH₄ rf plasma torch and an Ar-2%N₂ microwave discharge. Gas temperature as determined from CN and N₂ rotational svstems is 3200 ± 200 K in the rf torch and 700 ± 100 K in the post-discharge at a time 3 X10^–2 s after the rf plasma torch. From the intensities of the N₂ 1st positive system, of NO, and of CN violet hands, the atom densities have been determined as 2 X 10¹⁶ cm³ for N, 10¹⁵ cm³ for O, and 6 X 10¹² cm³ for C in the post-discharge at p=650 torr, with 10³ of CH₄ in the Ar torch.     

Fluorescence of Xe2 molecules in the vacuum-ultraviolet

Fluorescence of the Xe₂ continuum between 1460 and 1800 Å has been observed during excitation of Xe₂ molecules with CO fourth positive bands from a microwave discharge lamp. Fluorescence spectra at different Xe and added gas pressures show that in collisions with Xe or Kr atoms, the excited Xe₂ diatoms are efficiently relaxed to low vibrational levels of the ¹Σ_u⁺ and ³Σ_u⁺ potentials without being quenched noticeably. With Kr the rate constant for relaxation out of the primarily excited high vibrational levels is found to be about 3×10^?11 cm³ molecule^?1 s^?1.     

Glow discharge polymerization of tetramethyltin

Glow discharge polymerizations in the systems tetramethyltin (TMT), TMT/CH₄, TMT/C₂H₂ and TMT/N₂ were investigated and compared with those for methane and tetramethylsilane (TMS); some properties of the resulting polymers were examined. TMT is more easily polymerized in glow discharge than methane, and is deposited to as great an extent as TMS. Polymers prepared in these systems contain less carbon, nitrogen and oxygen than polymers from TMS; they consist mainly of CH₃, CH₂, CH, SnO and SnOSn groups. When nitrogen gas was mixed with TMT, amino groups were formed in the polymers. This formation arises from hydrolysis of SnN groups formed by interaction with TMT and nitrogen in glow discharge. This is distinctly different from the case of TMS. Surface energy, u.v. and visible absorption curve and thermal stability were measured. Adhesion between plasma films and polymer substrate is discussed.     

CN emission in active nitrogen. I. Enhanced violet emission at “low” microwave discharge power

Relative intensity measurements of CN violet emission in flowing, prepurified active nitrogen, both alone and in the presence of added mercury vapor, were obtained under a variety of microwave discharge power inputs. The results strongly suggest that excitation of ground state CN can be primarily attributed to collisional energy transfer from vibrationally excited N₂(X¹Σ_g⁺).