Excimer emission spectrum in noble gas systems

A simple expression for the time shape of excimer emission as a function of temperature is obtained for the case of a realistic (exponential) ground state potential. The excimer binding energy and its equilibrium geometry are obtained for the lowest ¹Σ_u states of Ar*₂, Kr*₂, Xe*₂ and for the A¹Σ_u and D¹Σ_u states of Hc*₂, by comparing the theoretical formula with the corresponding experamental results. Agreement with electronic calculations when available of these parameter is very good. The relation between our line-shape expression and those given by other authors is discussed.     

Through-space hydrogen-fluorine and carbon-fluorine spin-spin coupling in 5-fluoro-3,3-dimetryl-1,2,3,4-tetrahydrophenanthrene

The ¹R and ¹³C NMR spectra of the title compound ($\text{1}$) reveal through-space couplings between the fluorine and the C-4 methylene group ¹H and ¹³C), as well as coupling between the fluorine and the C-3 methine carbon and the C-2 methylene carbon.     

Tuning emission properties of iridium and ruthenium metallosurfactants in micellar systems

Ruthenium metallosurfactant forms micelles that show efficient electronic energy-transfer processes in the presence of an analogous iridium complex. Modulation of the process is achieved upon incorporation of these amphiphiles into cetyltrimethylammonium bromide micelles, allowing a tuning of the two emissions.     

Single molecule photon emission statistics of driven three-level systems

We study the statistics of photon emission from three-level single molecule systems. The generating function method [Y. Zheng and F. L. H. Brown, Phys. Rev. Lett. 90, 238305 (2003)] is used to calculate steady state absorption line shapes and Mandel's Q parameter as a function of excitation frequency, as well as the time dependence associated with approach to the steady state. The line shape calculations confirm known results derived via other methods, while the Q parameter results display complex frequency dependences not amenable to simple interpretation. This study confirms the applicability of the generating function formalism to multilevel quantum systems, including the proper modeling of quantum coherence effects.     

Synthesis and experimental study of through-space hydrogen-fluorine and carbon-fluorine spin-spin coupling in 4,5-substituted 1-acetyl-8-fluoronaphthalenes

The synthesis and NMR study (1H, 13C, and 19F) of a complete series of 4,5-substituted 1-acetyl-8-fluoronaphthalenes are reported. This data revealed a 6J(H,F) and a 5J(C,F) through space coupling between the fluorine and the methyl on the acetyl group (1H and 13C). The magnitude of this coupling constant changes depending on the nature of the substituent at C-4, the internuclear distance, and the solvent.     

Recombination of fragmented proteins

Directed evolution is a powerful method for generating novel molecules with desirable properties. In developing a new sensor to screen for protein-protein interactions, Tafelmeyer et al. report a clever strategy to evolve heterodimeric "split proteins" from a monomer in this issue of Chemistry & Biology.     

Recombination proteins and telomere stability in plants

Repair of DNA damage is essential for the maintenance of the integrity and transmission of the genome in development and reproduction. Telomeres are nucleoprotein structures which protect the ends of (linear) eukaryotic chromosomes. Telomere dysfunction results in loss of this protection and the telomeres being recognised as DNA damage by the cellular DNA Damage Repair and Response (DDR) machinery, leading to senescence or cell death. Telomeric homeostasis is thus tightly controlled and many specific and non-specific proteins are involved in its regulation. Among these, DNA damage and Repair proteins contribute both to the recognition of telomere dysfunction and more surprisingly, are directly implicated in telomere homeostasis itself. Plants offer a great opportunity to study these mechanisms due to the fact that many key DNA repair and recombination proteins are non-essential in plants, in contrast to vertebrates. In the following text, after a brief summary of the current state of knowledge on telomere-specific proteins in plants, we review the DDR processes and the related proteins implicated in plant telomere stability. We focus specifically on telomere signalling and on recombination events induced by unprotected telomeres, at the origin of genome rearrangements and instability when telomere function is affected.     

Recombination luminescence of poly(arylene phthalide) films: 2. Afterglow emission induced by electric excitation in poly(arylene phthalide) films

Absorption, luminescence and electroluminescence spectra of films of the unconjugated copolymer poly(arylene ether ketone) (CPAEK) were measured. Long-lasting afterglow emission was observed resulting from electro- and photoexcitation of the CPAEK films. and is possible mechanisms of generation are discussed.     

The Energy Barrier to Recombination in Hydrated Plasma

An abnormally high potential barrier that separates the H₃O⁺ and Cl^? ions in a cluster of water molecules was revealed. The profile of the barrier was calculated by computer simulation. The calculation was based on a detailed model of intermolecular interactions developed on the basis of experimental data on the free energy and entropy for the addition reactions of water molecules in the vapor phase to the hydration shell of ions in conjunction with the results of quantum-chemical calculations.     

Recombination of polyatomic ester peroxy radicals in solution

Termination rate constants of peroxy radicals of seven polyatomic esters in benzene and perflouorooctane media have been measured by pulse photolysis. Recombination of peroxy radicals for all esters examined proves to be diffusion controlled. Reactivity of peroxy radicals in the termination reaction grows with increasing number of ester groups.

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Recombination of iodine atoms in an unsteady expansion

Recombination of iodine atoms generated by shock heating I₂ in Ar is studied in an unsteady expansion. The three-body recombination rate coefficient has been measured as 3 × 10¹⁵ (T/298)^?1.56 cm⁶ mol^?2 s^?1 between 500 and 1450 K. Coupling of vibrational and chemical relaxation is found to occur in the expansion.     

Recombination of nanometric vesicles during freeze-drying

Concentrated dispersions of nanometric lipid vesicles (mean diameter 20 nm) in water/maltose solutions have been freeze-dried and then redispersed in water, yielding again dispersions of lipid vesicles. At each stage of the freeze-drying process, the organization of the vesicles in the dispersion and their size distribution were examined through small-angle neutron scattering and gel permeation chromatography. It was found that the osmotic deswelling of the vesicles caused them to recombine into larger vesicles. A single burst of recombination events occurred when the maltose concentration in the aqueous phase rose above 100 g/L. The final vesicle population was monopopulated, with a central diameter about twice as large as that of the original dispersion.     

Recombination of 1,1-dimethylpropyl peroxy radicals in polar solvents

The kinetics of 1,1-dimethylpropyl peroxy radicals recombination in polar solvents—water, methanol, and their mixtures—was studied by EPR spectroscopy in combination with the stopped-flow method, and the rate constants of this reaction were determined. Peroxyl radicals were generated by mixing solutions of Ce⁴⁺ sulfate and 1,1-dimethylpropyl hydroperoxide. The observed EPR signal of the peroxyl radical is a singlet with a g-factor of 2.015 ± 0.001, and a line width of ΔH = (1.36 ± 0.02) × 10^?3 T for methanol and ΔH = (9.7 ± 0.2) × 10^?4 T for water. The measured rate constants of (CH₃)₂C(O₂^·)CH₂CH₃ radical recombination at 298 K are 2k_t = (3.9 ± 0.4) × 10⁴ L mol^?1 s^?1 for water and 2k_t = (5.2 ± 0.5) × 10³ L mol^?1 s^?1 for methanol. A linear relationship between ln(2k_t) and the Kirkwood function (ε?1)/(2ε + 1), where e is the dielectric constant of the medium, has been established, indicating an important role of nonspecific solvation in the recombination of tertiary peroxyl radicals.     

Nature of the Transition State in Peroxyl Radical Recombination

We have carried out an ab initio calculation of the potential surface for the reaction CH₃O₄H CH₂=O + O₂ + H₂O. We have established the structure of the transition state and studied the dependence of the energy barrier on the size of the basis and whether electron correlation is taken into account. We have studied the electronically excited terms for the participants in this reaction and we have established the mechanism for the formation of chemiluminescence emitters in this reaction.     

Absolute emission cross sections for the calibration of optical detection systems in the 120–250 nm range

Absolute emission cross sections have been determined for electron impact on CO, NO and N₂. For the CO(A ¹ΠX ¹Σ⁺) and N₂(a ¹ΠX ¹Σ_g) radiation our data is in good agreement with that of other groups. For CO⁺ (B²Σ⁺X²Σ⁺) the values of the emission cross sections are different from those measured previously. This discrepancy is explained in terms of an inadequate straylight correction in the former experiments. For the NO(A²Σ⁺X²Π) emission no previous σ_em values are known to the authors. Furthermore the electronic transition moments of the NO(A²Σ⁺X²Π) and CO⁺(B²ΣX²Σ⁺) systems have been measured and are found to be independent of the internuclear distance.