26 resultados para EXCITED HYPERONS
em Scielo Saúde Pública - SP
Resumo:
Photoacoustic spectroscopy provides information about both amplitude and phase of the response of a system to an optical excitation process. This paper presents the studies of the phase in the electron transfer process between octaethylporphyn (OEP) and quinone molecules dispersed in a polymeric matrix. It was observed a tendency in the phase behavior to small values only in the spectral region near to 620 nm, while for shorter wavelength did not show any tendency. These measurements suggested that the electron transfer to acceptor occurred with the participation of octaethylporphyn singlet excited state.
Resumo:
The author has studied the influence of acetylcholine solutions directly applied on the motor cortex of dogs, cats monkeys and rabbits. For this purpose small squares of filter paper were soaked in the acetylcholine solution and soon afterwards laid on the motor cortex. Solutions varying from 0,2 to 10 per cent have been experimented. It has been shown that local application of the solutions on the motor points, previously localized by induction coil, produced motor reactions. It has been found, in the dogs that 10 per cent acetylcholine solutions cause localized muscular twitchings (clonus) in almost all the animals experimented. Generalised epileptiform convulsions were obtained in44,4% of the dogs. Convulsions were also obtained by employing 1 per cent solution of acetylcholine. Definite response has been obtained with 0,2 per cent solution. Failure of motor action, pointed out by other authors, has been related to the use of anesthetics. Convulsions were easily produced by rapid light mechanical stimulations of the skin covering the muscles in conection with the excited motor point, and the application on the motor point of acetylcholine. The results on monkeys can be summarized as follows. Two species of monkeys were experimented: Cebus capucinus and Macaca mulata. In the monkeys C. capucinus generalised convulsive reactions were induced with actylcholine solutions in a concentration as low as 0,5 per cent. Motor reaction or convulsive seizeres were obtained in seven of the eight monkeys used. Three monkeys M. mulata were stimulated with 10 per cent acetylcholine solution but only localized muscular contraction hae been observed. Similar results has been obtained on the motor cortex of cats and rabbits. One of the three cats employed has shown epileptiform convulsions and the remaining only localized muscular contractions. In the rabbits muscular twitchings have been also induced. The sensitizing power of eserine on the action of acetylcholine has been also searched. The results indicate that a previous application of eserine solution on the motor center, potentiates the action of acetylcholine. The intensity of the muscular twitchings is greater than the obtained before the application of the eserine solution. Generalised epileptiform convulsions sometimes appeared following the use of lower concentrations of acetylcholine than those previously employed. Experiments have been carried out by injecting eserine and prostigmine by parenteral route. A dosis dufficient for induce small muscular tremors did not enhance obviously the motor effects produced by the application of the acetylcholine solutions on the motor cortex. From seven dogs experimented, all previously tested for convulsive seiruzes by application of 1 and 10 per cent acetylcholine solution with negative results, only one has shown epileptiform convulsions after the injection of prostigmine. Morphine has also been tested as facilitating substance for convulsions induced by acetylcholine. Six from the nine dogs submitted to the experiments, developed epileptiform seizures after injection of morphine and stimulation of the motor cortex with acetylcholine. (Table IV). In another series of experiments atropine and nicotine have been studied as for to their action on the motor effects of acetylcholine. Nicotine has a strong convulsant action, even when employed in very high concentration. Since a depressant effect has not appeared even by the applications of high concentrations of nicotine in the motor corteõ of dogs, unlike the classical observations for the autonomus nervous system, it was not possible to verify the action of acetylcholine on a motor center paralised by nicotine. It is important to not that the motor phenomena observed after the first aplication of acetylcholine, can desappear by the renewal of the pieces of filter paper soaked in the acetylcholine solution. Atropine, either applied on the motor point in low concentration, or injected in sufficient amount for inhibiting the muscarinic effects of acetylcholine on the autonomous nervous system, did not prevent the motor reactions of acetylcholine on the cerebral cortex.
Resumo:
A general overview on the photochemical behaviour of [Ru(NH3)5L]2+ complexes (where L is a p ligand) is presented. The proposed mechanisms and techniques employed for the study of these reactions are discussed. Emphasis is made on the mechanisms that allow the identification of the reactive excited state of the [Ru(NH3)5py]2+ complex.
Resumo:
Angle-resolved electron energy-loss spectra have been measured for the methyl methacrylate (MMA) and styrene molecules in the 0 - 50 eV energy range. The spectra have been obtained at 1 keV incident energy, with an energy resolution of 0.8 eV and covering an angular range of 2.0 to 7.0 degrees. Within our knowledge, this is the first gas-phase excitation spectrum for MMA and styrene in this energy range. The spectra of MMA at small scattering angles are dominated by an intense peak at 6.7 eV followed by a broad band centered at about 16 eV. In the case of styrene, six bands can be observed in the spectra. Based on the angular behaviour of the excitation spectra of these molecules, the low-lying peaks observed are considered to be associated predominantly with dipole-allowed processes. In both cases, new bands can be observed for excitation energies greater than 20 eV. This could be associated with dipole-forbidden transitions to shake-up and doubly-excited states.
Resumo:
This review has tried to collect and correlate all the various equations for the g matrix of strong field d5 systems obtained from different basis sets using full electron and hole formalism calculations. It has corrected mistakes found in the literature and shown how the failure to properly take in symmetry boundary conditions has produced a variety of apparently inconsistent equations in the literature. The review has reexamined the problem of spin-orbit interaction with excited t4e states and finds that the earlier reports that it is zero in octahedral symmetry is not correct. It has shown how redefining what x, y, and z are in the principal coordinate system simplifies, compared to previous methods, the analysis of experimental g values with the equations.
Resumo:
The generation of "cold light", visible to the human eye, by chemical reactions has attracted the attention of the scientific community since the beginning of this century. Besides the academic interest in the elucidation of the mechanisms of excited state formations, many chemiluminescence reactions have found widespread analytical applications. Moreover, the phenomenon of chemiluminescence can also be used as a tool in undergraduate and college teaching. In this article, we describe several known chemiluminescence demonstrations, which are suitable for school teaching. The main objective of this work is to produce didactic material in Portuguese to stimulate Brazilian secondary and high school teachers to use these experiments in the classroom. The demonstrations include singlet oxygen emission, the luminol reaction, oscillating chemiluminescence and the peroxyoxalate reaction.
Resumo:
The initiation step of the light-induced polymerization kinetics of vinyl monomers using dye-sensitized photoinitiators to generate active radicals is discussed. The photoredox processes of basic dyes with amines and sulfinates are described as photochemical systems capable of starting free-radical polymerization of vinyl monomers in homogeneous and microheterogeneous media. Photophysical techniques like laser flash photolysis and time-correlated single photon counting are used to investigate the excited-state kinetics of the dyes.
Resumo:
Laser excitation of 0.01 M solutions of 1-indanone (Ia), 1-tetralone (Ib), 1-benzosuberone (Ic), and their a,a -dimethyl derivatives IIa-c, respectively, in benzene, produced transients with maximum absorption at 425 nm, and lifetimes ranging from 62 ns (IIa) to 5.5ms (Ic). Quenching studies using well known triplet quenchers such as 1,3-cyclohexadiene and oxygen demonstrated the triplet nature of these transients. In the presence of hydrogen donors, such as 2-propanol, the triplet state decay of the ketones Ia-c leads to the formation of the corresponding ketyl radicals, i.e. IIIa-c, which show absorption spectra very similar to the parent ketone, with lmax at 430 nm and lifetime in excess of 20 ms. Steady state irradiations show that the a,a -dimethyl ketones IIa and IIc form ortho-alkyl benzaldehydes probably derived from an initial a-cleavage of the corresponding triplet excited states.
Resumo:
Molecular oxygen, in the first excited state (singlet oxygen, ¹O2), has a substantial reactivity towards electron-rich organic molecules, such as biological targets, including unsaturated fatty acids, proteins, RNA and DNA. Considering the complexity of biological systems and the great variety of reactive species generated by photochemistry, efforts have been devoted to develop suitable ¹O2 generators based on the thermolysis of water soluble naphthalene endoperoxides. These compounds are chemically inert and have been employed as versatile sources of ¹O2. The synthesis is based on structural modifications in position 1,4 of dimethylnaphtalene, grafting hydrophilic substituents. The correspondent endoperoxide can be generated using photochemical method, or molybdate-catalyzed disproportionation of hydrogen peroxide.
Resumo:
The photofragmentation of a core-excited halogenated compound, Halotane (C2F3HClBr), generally used as anesthetic by inhalation, has been studied using high energy photons and electrons near C 1s ionization edge (~ 300 eV), using time-of-flight mass spectrometry in multicoincidence mode. We observe strong differences between the molecular fragmentation induced by photons and electron impact.
Resumo:
In this review article, we give a general introduction on the mechanisms involved in organic chemiluminescence, where three basic models for excited state formation are presented. The chemiluminescence properties of 1,2-dioxetanes - four membered ring peroxides - are briefly outlined in the second part. In the main part, the mechanisms involved in the decomposition of 1,2-dioxetanes and analogous peroxides are discussed: (i) the unimolecular decomposition of 1,2-dioxetanes; (ii) the electron transfer catalyzed decomposition of peroxides by an intermolecular CIEEL (Chemically Initiated Electron Exchange Luminescence) mechanism; (iii) 1,2-dioxetane decomposition catalyzed by an intramolecular electron transfer mechanism (intramolecular CIEEL). Special emphasis is given to the latter subject, where recent examples with potential analytical applications are presented.
Resumo:
Rate constants for the quenching of 1,3-indandione (1) triplet by olefins and by hydrogen and electron donors were obtained employing the laser flash photolysis technique in benzene solution. These rate constants ranged from 2.5x10(5) Lmol-1s-1 (for 2-propanol) to 5.9x10(9) Lmol-1s-1 (for DABCO). From the quenching rate constants by 1,3-cyclohexadiene, trans- and cis-stilbene a value between 49.3 and 52.4 kcal/mol was estimated for the energy of the triplet state of 1,3-indandione. The npi* character of this triplet state was evidenced by the quenching rate constants obtained when typical hydrogen donors were employed as quenchers. For 2-phenyl-1,3-indandione (2, R=phenyl) a fast Norrish type I reaction is operating which prevents the determination of kinetic and spectroscopic data of its triplet state.
Resumo:
Iodine vapor is a very suitable substance to learn about molecular energy levels and transitions, and to introduce spectroscopic techniques. As a diatomic molecule its spectra are relatively simple and allow straightforward treatment of the data leading to the potential energy curves and to quantum mechanics concepts. The overtone bands, in the resonance Raman scattering, and the band progressions, in the electronic spectra, play an important role in the calculation of the Morse potential curves for the fundamental and excited electronic state. A weaker chemical bond in the electronic excited state, compared to the fundamental state, is evidenced by the increase in the equilibrium interatomic distance. The resonance Raman scattering of I2 is highlighted due to its importance for obtaining the anharmonicity constant in the fundamental electronic state.
Resumo:
Rare earth ion doped solid state materials are the most important active media of near-infrared and visible lasers and other photonic devices. In these ions, the occurrence of Excited State Absorptions (ESA), from long lived electronic levels, is commonplace. Since ESA can deeply affect the efficiencies of the rare earth emissions, evaluation of these transitions cross sections is of greatest importance in predicting the potential applications of a given material. In this paper a detailed description of the pump-probe technique for ESA measurements is presented, with a review of several examples of applications in Nd3+, Tm3+ and Er3+ doped materials.
Resumo:
The effect of the introduction of nitrogen atoms upon the triplet excited state reactivity of 1,4-diaza-9-fluorenone (1) and 1,4-diaza-9-benz[b]fluorenone (2), in acetonitrile, was investigated employing the nanosecond laser flash photolysis technique. The intersystem crossing quantum yield (Φces) for 1 and 2 was determined using 9-fluorenone as a secondary standard (Φces= 0.48, in acetonitrile) and for both diazafluorenones a value of Φces= 0.28 was found. Quenching rate constants ranged from 8.17x10(4) L mol-1 s-1 (2-propanol) to 1.02x10(10) L mol-1 s-1 (DABCO) for 1,4-diaza-9-fluorenone and from 6.95x10(5) L mol-1 s-1 (2-propanol) to 5.94x10(9) L mol-1 s-1 (DABCO) for 1,4-diaza-9-benz[b]fluorenone, depending if the quenching process involves energy, hydrogen or electron transfer. A comparison between quenching rate constants for both diazaflurenones and the parent compound, i.e. 9-fluorenone, a ketone with lowest triple state of ππ* configuration, lead to the conclusion that the reactive triplet excited state for 1,4-diaza-9-fluorenone and 1,4-diaza-9-benz[b]fluorenone has ππ* configuration.