Drift study of the products formed by radiolysis and photolysis of alkaline nitrates

The products of the radiolysis and photolysis of crystalline sodium, potassium, rubidium, cesium nitrates have been investigated by the diffuse reflectance infrared Fourier transform spectroscopy. The bands in the 1260-1220 and 804-809 cm^?1 regions observed after the n -irradiation and photolysis by a light with the wave length 253.7 nm of crystalline alkali nitrates were identified as the vibrational modes of NO^? ₂ x ₃ and x ₂, respectively. The frequency of the x ₃ oscillation of nitrite ions decreases from 1260 cm^?1 up to 1220 cm^?1 with the increase of the atomic weight or polarizability of a cation. The detection limit of the nitrite ions (1 ‐ 10^?7 mol g^?1) for the diffuse reflection method has been determined. The bands observed in KNO₃, RbNO₃ and CsNO₃ spectra in the 947-940 and 722-737 cm^?1 regions appearing only after photolysis are due to stretch oscillations of the peroxide bond O-O and wagging oscillations of the -ON=O group of peroxynitrite accordingly.     

Quantum chemical molecular dynamical investigation of alkyl nitrite photo-dissociated on copper surfaces

An accelerated quantum chemical molecular dynamical code “Colors-Excite” was used to investigate the photolysis of alkyl nitrites series, RONO (RCH₃ and C(CH₃)₃) on copper surfaces. Our calculations showed that the photo-dissociated processes are associated with the alkyl substituents of RONO when adsorbed on copper surfaces. For RCH₃, a two-step photolysis reaction occurred, yielding diverse intermediate products including RO radical, NO, and HNO, consistent with those reported in gas phase. While for RC(CH₃)₃, only one-step photolysis reaction occurred and gave intermediate products of RO radical and NO. Consequently, pure RO species were achieved to adsorb on metal surfaces by removing the NO species in photolysis reaction. The detailed photo-dissociated behaviors of RONO on copper surfaces with different alkyl substituents which are uncovered by the present simulation can be extended to explain the diverse dissociative mechanism experimentally observed. The quantum chemical molecular dynamical code “Colors-Excite” is proved to be highly applicable to the photo-dissociations on metal surfaces.     

A polarized CARS investigation of the fine structure population inversion of Cl atoms from laser photolysis of ICl and the quenching of Cl(2 P 1/2) by O2

The time resolved polarized CARS technique has been used to detect Cl atoms produced by photolysis of ICl in the presence and absence of O₂. A population inversion was observed between the ground state electronic levels Cl(² P _1/2) and Cl(² P _3/2). The rate constant for Cl(² P _1/2) decay (quenching + reaction) in ICl was determined to be (3.2±0.2)×10^–13 cm³/molecule×s; the rate constant for Cl(² P _3/2) reaction with ICl was determined to be (7.8±0.5)×10^–12 cm³/molecule×s; and the rate constant for Cl(² P _1/2) quenching by O₂ was determined to be (1.9±0.2)×10^–13 cm³/molecule×s.     

Chemically Induced Dynamic Magnetic Polarization. Part X. The Photoreduction of 2-Methyl-p-benzoquinone

While the photoreduction of quinones has been initially used by us as a model system to probe the role of excited triplet states in CIDEP¹ and CIDNP² phenomena, our continuing interest in the quinone photochemical systems is partly due to their photobiological importance. Alkyl substituted quinones have in fact been shown to be associated with chlorophyll³ and to be involved in photosynthesis⁴. The 2-methyl-p-benzoquinone (MQ) is the simplest unsymmetrical alkyl substituted p-quinone which, during photolysis, may lead to two isomeric semiquinone radicals. We are particularly interested in applying the CIDEP and CIDNP techniques to investigate the structure and reactivity of the intermediate semiquinone radicals as they may give some insight to the photochemical properties of the parent 2-methyl-p-quinone.     

Matrix isolation study of the infrared spectrum of thioformaldehyde

H₂CS has been trapped in argon and nitrogen matrices at 14 K as a product of the pyrolysis of s-trithiane or (CH₃S)₂ and of the ultraviolet or vacuum ultraviolet photolysis of CH₃SH. A small concentration of H₂CS has also been observed upon vacuum ultraviolet photolysis of a mixture of CH₄ and H₂S in an argon matrix. The isotopic data support the assignment of absorptions at 993 and at 1063 cm^?1 to the out-of-plane deformation and the CS stretching fundamentals of H₂CS. Absorptions in the CH stretching region which were assigned to H₂CS in an earlier gas-phase study were confirmed in the matrix experiments. Studies of the vacuum ultraviolet photolysis of CD₃SH have provided information on the mechanism of the photolysis process.     

Excited Atoms in the Flash Photolysis of some Germanium Compounds

We have recently reported measurements of the rates of the collisional relaxation of various atoms amongst the spin-orbit components of their ground electronic states; an approximate correlation exists with other types of molecular energy transfer.^1-3 We present here an outline of some qualitative observations of the production and relaxation of Ge(4¹D₂) and Ge(4³P_j) in the flash photolysis of a number of germanium compounds. Atomic germanium vas selected for study because the ground state comprises a ‘normal’ Landé multiplet and should exhibit ‘Inverted’ relaxation as compared for example to Fe(a⁵D_j) which equilibrates initially in the high energy substates. The low lying states of germanium are listed In table 1.⁴ The flash photolysis apparatus was of standard design^1-3 and spectra were recorded with a Hilger medium quartz spectrograph.     

Synthesis of functionalized pyrrole derivatives via diverse cyclization of azomethine ylide and olefins

The azomethine ylides are generally used in 1,3-dipolar cycloadditions with various dipolarophiles. In this work, a new and diverse route has been developed for the azomethine ylides, for synthesis of novel pyrrole derivatives. The azomethine ylide, produced via C–H activation of unreactive C(sp³)–H bond of 2-methylquinoline, by molecular iodine, in the presence of pyridine. Herein, we represent novel pyrrole derivatives, synthesized from the reaction of pyridinium ylide with olefins, which formed via a reaction of isatin, dialkyl acetylenedicarboxylate derivatives and pyridine as a base in moderate to excellent yields. Various features of this cyclization, discussed.

Graphic abstract

     

Atomistic computer simulation studies of La1−xSrxVO3

Static computer simulation techniques have been employed for structural investigation of the La_1−xSr_xVO₃ series. Potential parameters for V³⁺-O²⁻ and V⁴⁺-O²⁻ have been derived which reproduces the crystal structures of end members with sufficient accuracy. Variations of lattice parameters and bond distances with Sr concentration have been studied. The calculated lattice parameters decrease with increase in the Sr concentration. A structural phase transition from orthorhombic to cubic is observed at 50% Sr doping level.     

Near infrared cw-CRDS coupled to laser photolysis: Spectroscopy and kinetics of the HO2 radical

We present in this work a new experimental set-up for sensitive detection of reactive species: continuous wave cavity ring-down spectroscopy (cw-CRDS) as a detection method in laser photolysis reactor. HO₂ radicals were generated by using a 248 nm photolysis of SOCl₂/CH₃OH/O₂ mixtures and were detected in the first vibrational overtone of the OH stretch around 6625 cm^-1, using a DFB diode laser. In order to perform the spectroscopic and kinetic measurements of the HO₂ radical, two different timing schemes have been used. The absorption line strength of the transition at 6625.784 cm^-1 has been extracted from kinetic measurement to (5.2±1.0)×10^-21 cm² molecule^-1cm^-1. The detection limit for the actual set-up is 2×10¹² molecules cm^-3. PACS 42.62.Fi; 82.33.Tb; 82.20.W     

1,5‐electrocyclization versus 1,5‐proton shift in imidazolium allylides and 2‐phospha‐allylides: a DFT investigation

The competitive 1,5‐electrocyclization versus intramolecular 1,5‐proton shift in imidazolium allylides and imidazolium 2‐phosphaallylides has been investigated theoretically at the DFT (B3LYP/6‐311 + +G**//B3LYP/6‐31G**) level. 1,5‐Electrocyclization follows pericyclic mechanism and its activation barrier is lower than that for the pseudopericyclic mechanism by ～5–6 kcal mol^?1. The activation barriers for 1,5‐electrocyclization of imidazolium 2‐phosphaallylides are found to be smaller than those for their nonphosphorus analogues by ～3–5 kcal mol^?1. There appears to be a good correlation between the activation barrier for intramolecular 1,5‐proton shift and the density of the negative charge at C8, except for the ylides having fluorine substituent at this position ( 7b and 8b ). The presence of fluorine atom reduces the density of the negative charge at C8 (in 7b it becomes positively charged) and thus raises the activation barrier. The ylides 7f and 8f having CF₃ group at C8, in preference to the 1,5‐proton shift, follow an alternative route leading to different carbenes which is accompanied by the loss of HF. The carbenes Pr _{7 , 8b – e} resulting from intramolecular 1,5‐proton shift have a strong tendency to undergo intramolecular S_N2 type reaction, the activation barrier being 7–28 kcal mol^?1. Copyright © 2011 John Wiley & Sons, Ltd.     

Infrared diode laser kinetic spectroscopy of transient molecules produced by excimer laser photolysis: Application to the SO radical

Excimer laser photolysis has been incorporated with infrared tunable diode laser spectroscopy in order to observe infrared spectra, primarily vibration-rotation spectra, of transient molecules which are difficult to produce by other means such as electrical discharge. The method has been applied to SO generated by the photolysis of SO₂, and the vibration-rotation transitions of SO in the X³Σ^? state, each resolved into a fine structure triplet, have been identified for the bands of v = 1?0 up to 6?5 and have been analyzed to improve the precision of the vibrational parameters.     

NMR Studies of Hindered Rotation. The Diels-Alder Adduct of Phencyclone with Maleic Anhydride: Restricted Motion of Bridgehead Phenyls

¹H NMR studies at 300 MHz have been performed for the Diels-Alder adduct of phencyclone and maleic anhydride in CDCl₃ at ambient temperatures. The 1D spectrum shows four equal (2H) intensity doublets in the aryl region (in addition to other absorptions) which is fully consistent with a slow exchange limit (SEL) spectrum of a system in which the unsubstituted bridgehead phenyls exhibit hindered rotation around the C(sp²)-C (sp³) bond on the NMR timescale. These protons are assigned to H-1,8 and H-4,5 of the phenanthrene moiety and to H-2′ and H-6′ of the phenvls based on the two-dimensional (2D) homonuclear chemical shift correlation spectrum (COSY) together with arguments regarding carbonyl and aromatic ring anisotropy. Full proton assignments are given.     

Keith E. Gubbins: A celebration of statistical mechanics

We have used the density functional B3LYP method to study the effect of hydrogen bonds from the histidine ligand in various haem proteins to carboxyl groups or to the carbonyl backbone. Hydrogen bonds to carbonyl groups (encountered in globins and cytochromes, for example) have a small influence on the geometry and properties of the haem site. However, hydrogen bonds to a carboxyl group (encountered in peroxidases and haem oxidase) may have a profound effect. The results indicate that in the Fe³⁺ state, this leads to a deprotonation of the histidine ligand, whereas in the Fe²⁺ state, the proton involved in the hydrogen bond may reside on either histidine or the carboxylate group, depending on the detailed structure of the surroundings. If the histidine is deprotonated, the axial Fe-N bond length decreases by 0.15 Å, whereas the equatorial bond lengths increase. Moreover, the charge on iron and histidine is reduced, as is the spin density on iron. Most importantly, the energy difference between the high and intermediate spin states changes so that whereas the two spin states are degenerate in the Fe²⁺ state for the protonated histidine, they are degenerate for the Fe³⁺ state when it is deprotonated. This may facilitate the spin-forbidden binding of dioxygen and peroxide substrates, which takes place for the Fe²⁺ state in globins but in the Fe³⁺ state in peroxidases. The reduction potential of the haem group decreases when it hydrogen-bonds to a negatively charged group. The inner-sphere reorganization energy of the Fe²⁺/Fe³⁺ transition in a five-coordinate haem complex is ～30 kJ mol^?1, except when the histidine ligand is deprotonated without any hydrogen-bond interaction.     

NMR Studies of Drugs. Applications of Lanthanide Shift Reagents to Afloqualone,an Axially Chiral Quinazolinone.

The skeletal muscle relaxant, aflogualone, 1, has been studied by ¹H NMR in CDC1₃ at 60 and 300 MHz in the presence of added chiral [Eu(HFC)₃] or achiral [Eu(FOD)₃] lanthanide shift reagents (LSR). With Eu(HFC)₃, significant enantiomeric shift differences, ΔΔδ, can be induced for most of the nuclei of 1, with near-baseline resolution obtainable for the H-5 signals of each enantiomer, indicating excellent analytical potential for direct determination of enantiomeric excess of samples of 1. Observation of ΔΔδ directly confirms hindered rotation about the bond between N (3) and the 2-methylphenyl group, i.e., the N (sp²) - C(sp²) bond, leading to axial chirality in 1 with slow rotation on the NMR timescale. Assignments are supported by 2D COSY spectra at 300 MHz. Relative lanthanide-induced shift magnitudes for the protons of 1 are compared.     

Thermolysis and photolysis of 2‐ethyl‐4‐nitro‐1(2H)‐isoquinolinium hydroperoxide

The thermal and light‐induced O ? O bond breaking of 2‐ethyl‐4‐nitro‐1(2H)‐isoquinolinium hydroperoxide (IQOOH) were studied using ¹H NMR, steady‐state UV/vis spectroscopy, femtosecond UV/vis transient absorption (fs TA) and time‐dependent density functional theory (TD DFT) calculations. Thermal O ? O bond breaking occurs at room temperature to generate water and the corresponding amide. The rate of this reaction, k = 5.4 · 10^?6 s^?1, is higher than the analogous rates of simple alkyl and aryl hydroperoxides; however, the rate significantly decreases in the presence of small amounts of methanol. The calculated structure of the transition state suggests that the thermolysis is facilitated by a 1,2 proton shift. The photochemical process yields the same products, as confirmed using NMR and UV/vis spectroscopy. However, the quantum yield for the photolysis is low (Φ = 0.7%). Fs TA studies provide additional detail of the photochemical process and suggest that the S₁ state of IQOOH undergoes fast internal conversion to the ground state, and this process competes with the excited‐state O ? O bond breaking. This result was supported by the fact that the model compound IQOH exhibits similar excited‐state decay lifetimes as IQOOH, which is assigned to the S₁ → S₀ internal conversion. Copyright © 2013 John Wiley & Sons, Ltd.     

Chemical reaction of sputtered Cu film with PI modified by low energy reactive atomic beam

Polyimide (PMDA-ODA) surface was irradiated by low energy reactive atomic beam with energy 160-180 eV to enhance the adhesion with metal Cu film. O₂⁺ and N₂⁺ ions were irradiated at the fluence from 5 × 10¹⁵ to 1 × 10¹⁸ cm⁻². Wetting angle 78° of distilled deionized (DI) water for bare PI was greatly reduced down to 2-4° after critical ion flounce, and the surface energy was increased from 37 to 81.2 erg/cm. From the analysis of O 1s core-level XPS spectra, such improvement seemed to result from the increment of hydrophilic carbonyl oxygen content on modified PI surface. To see more carefully correlation of the peel strength with interfacial reaction between Cu and PI, flexible copper clad laminate with Cu (9 μm)/Cu (200 nm) on modified PI substrate (25 μm) was fabricated by successive sputtering and electroplating. Firstly, peel strength was measured by using t-test and it was largely increased from 0.2 to 0.5 kgf/cm for Ar⁺ only irradiated PI to 0.72-0.8 kgf/cm for O₂⁺ or N₂O⁺ irradiated PI. Chemical reaction at the interface was reasoned by analyzing C 1s, O 1s, N 1s, and Cu 2p core-level X-ray photoelectron spectroscopy over the as-cleaved Cu-side and PI side surface through depth profiling. From the C 1s spectra of cleaved Cu-side, by the electron transfer from Cu to carbonyl oxygen, carbonyl carbon atom became less positive and as a result shifted to lower binding energy not reaching the binding energy of C₂ and C₃. The binding energy shift of the peak C₄ as small as 1.7 eV indicates that carbonyl oxygen atoms were not completely broken. From the analysis of the O 1s spectra, it was found that new peak at 530.5 eV (O₃) was occurred and the increased area of the peak O₃ was almost the same with reduced area of the peak carbonyl oxygen peak O₁. Since there was no change in the relative intensity of ether oxygen (O₂) to carbonyl oxygen (O₁), and thus O₃ was believed to result from Cu oxide formation via a local bonding of Cu with carbonyl oxygen atoms. Moreover, from X-ray induced Auger emission spectra Cu LMM which was very sensitive to chemical bonding, Cu oxide or CuOC complex formation instead of CuNO complex was clearly identified by the observation of the peak at 570 eV at higher 2 eV than that of metal Cu. In conclusion, when Cu atoms were sputtered on modified PI by low energy ion beam irradiation, it can be suggested that two Cu atoms locally reacted with carbonyl oxygen in PMDA units and formed Cu⁺O⁻C complex linkage without being broken from carbon atoms and thus the chemically bound Cu was in the form of Cu₂O.     

Magnetic properties of thick multiferroic hexagonal HoMnO3 films

Multiferroic hexagonal HoMnO₃/YSZ(1 1 1) films with a thickness of ?1 μm have been grown by pulsed laser deposition. Conventional X-ray diffraction and pole figure measurement indicate that the film is epitaxially grown without secondary phase or misorientation. Magnetization measurements reveal some differences in comparison with a single crystal. These differences are possibly related to the larger a and c lattice parameters of the film which are likely to alter the bond lengths and, thus, the magnetic superexchange interactions. A substantial change of the complex Ho³⁺ magnetic ordering below 6 K is observed.     

Doping mechanism of optical-damage-resistant ions in lithium niobate crystals

The doping mechanism of optical-damage-resistant ions (Mg²⁺, Zn²⁺, In³⁺, Sc³⁺, Hf⁴⁺, and Zr⁴⁺) in the lithium niobate crystallographic frame is quantitatively studied from the chemical bond viewpoint. Calculated results show that optical-damage-resistant ions have a strong interaction with the lithium niobate matrix, which is quantitatively evaluated by the deviation between normal and calculated valence states and the global instability index. All optical-damage-resistant ions first substitute Nb_Li and then Li ions, they change their dopant occupancies from Li to Nb sites at the same global instability index value 0.1055. On the basis of such a quantitative interaction, the doping mechanism of these ions is finally derived. Furthermore, a criterion in searching for new optical-damage-resistant ions is also proposed.     

The assignment of Co-C bond stretching vibrational frequency of CH3Co(DH)2H2O in IR and Raman spectra

Abstract

In order to aid assignment of Co-C bond stretching vibrational frequency of CH₃Co(DH)₂H₂O (DH=dimethylgIyoximato monanion) in IR and Raman spectra, its isotopic substitution CD₃Co(DH)₂H₂O has been synthesized and normal coordinate analyses on the two complex have been made. The bands were assigned in terms of potential energy distribution. The results provide definitive band assignment of the Co-C bond and Co-N bond stretching modes which are coupling at 511 cm^?1.     

Density functional study of uranyl （VI） amidoxime complexes

Uranyl (VI) amidoxime complexes are investigated using relativistic density functional theory. The equilibrium structures, bond orders, and Mulliken populations of the complexes have been systematically investigated under a generalized gradient approximation (GGA). Comparison of (acet) uranyl amidoxime complexes ([UO₂(AO)_n]^2-n, 1 ≤ n ≤ 4) with available experimental data shows an excellent agreement. In addition, the U-O(1), U-O(3), C(1)-N(2), and C(3)-N(4) bond lengths of [UO₂(CH₃AO)₄]^2- are longer than experimental data by about 0.088, 0.05, 0.1, and 0.056 Å. The angles of N(3)-O(3)-U, O(2)-N(1)-C(1), N(3)-C(3)-N(4), N(4)-C(3)-C(4), and C(4)-C(3)-N(3) are different from each other, which are due to existing interaction between oxygen in uranyl and hydrogen in amino group. This interaction is found to be intra-molecular hydrogen bond. Studies on the bond orders, Mulliken charges, and Mulliken populations demonstrate that uranyl oxo group functions as hydrogen-bond acceptors and H atoms in ligands act as hydrogen-bond donors forming hydrogen bands within the complex.