987 resultados para 7 (2 hydroxyethyl)guanine


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介绍了一种高重复频率掺钛蓝宝石飞秒激光多通高效率放大系统.在抽运功率为23W,入射功率为660mW时,获得7.2W的放大输出,放大效率达30%.经压缩器压缩后,获得单脉冲能量4.5mJ,脉冲宽度为38fs,重复频率为1kHz,峰值功率大于0.1TW的超短超强激光脉冲.

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The 45 degrees scattering of a femtosecond (60 fs) intense laser pulse with a 20 nm FWHM (the full width at half maximum) spectrum centered at 790 nm has been studied experimentally while focused in argon clusters at intensity similar to 10(16) W/cm(2). Scattering spectra under different backing pressures and laser-plasma interaction lengths were obtained, which showed spectral blueshifting, beam refraction and complex modulation. These ionization-induced effects reveal the modulation of laser pulses propagating in plasmas and the existing obstacle in laser cluster interaction at high laser intensity and high electron density.

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Under coronal conditions, the steady state rate-equations are used to calculate the inter-stage line ratios between Li-like Is(2)2p(P-2(3/2))-> 1s(2)2s -> ((2) S-1/2) and He-like 1s2p (P-1(1))-> 1s(2) (S-1(0)) transitions for Ti in the electronic temperature ranges from 0.1 keV to 20 keV. The results show that the. temperature sensitivities are higher at the electronic temperature less than 5000 eV and the temperature sensitivities will decrease with the increase of electronic temperature.

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Não tem sido frequentes no Brasil estudos de avaliação da qualidade dos serviços de saúde. Tem sido adotado entendimento de qualidade como o grau em que processo de assistência aumenta a probabilidade de resultados favoráveis e diminui a probabilidade de resultados desfavoráveis, dado o estado do conhecimento médico. Indicadores de resultados de efeitos adversos do processo de assistência costumam ser empregados e, entre eles, para aquelas condições e procedimentos onde óbitos ocorrem com frequência, estão as taxas de mortalidade hospitalar. Entre esses procedimentos inclui-se a cirurgia de revascularizaçäo do miocárdio. Apesar de frequentes na literatura, particularmente norte-americana, não há estudos de escala realizados no Brasil. Para estudos deste tipo bases de dados administrativas tem sido empregadas. No Brasil recentemente tem sido exploradas as potencialidades dos bancos de dados do Sistema de Informações Hospitalares do Sistema Único de Saúde do Ministério da Saúde (SIH-SUS) em diversos estudos. Como há registro de óbitos hospitalares no sistema é possível utilizá-lo para a obtenção de dados sobre mortalidade hospitalar. Os bancos de dados do SIH-SUS de 1996 a 1998 foram integrados e as variáveis disponíveis no banco obtido examinadas quanto a possibilidade de inclusão do estudo descritivo de características da cirurgia coronária no país. Foram identificadas aquelas variáveis que poderiam ser utilizadas para proceder algum grau de ajuste de risco para os casos atendidos pelos diferentes hospitais. Para que se obtivesse uma comparação do comportamento do ajuste obtido com essas variáveis com modelos mais completos que incorporassern mais variáveis, inclusive variáveis clínicas, foram estudadas para o mesmo período, as internações realizadas no Hospital Universitário Pedro Ernesto da Universidade do Estado do Rio de Janeiro, utilizando dados de banco específico do Serviço de Cirurgia Cardíaca. Além do estudo descritivo foram desenvolvidos para os casos deste hospital modelos de regressão logística incorporando variáveis pré-operatórias e com as variáveis disponíveis no SIH-SUS para avaliar as diferentes capacidades de ajuste de risco. Após a escolha de um modelo de risco com maior capacidade de ajuste, foram calculadas as taxas de mortalidade hospitalar e obtidos os valores de taxas esperadas após o ajuste de risco. Os hospitais forma ordenados de acordo com as razões entre as taxas observadas e esperadas e identificados aqueles hospitais que apresentavam razões estatisticamente significativas superiores e inferiores a média nacional. Estudou-se também o efeito do volume de casos sobre a mortalidade hospitalar. Foram obtidas informações de 41.989 cirurgias codificadas como cirurgia coronária com circulação extracorpórea realizadas em 131 hospitais brasileiros, em 22 unidades da federaçâo. A taxa anual por 100000 habitantes foi de 8,7 para o Brasil, com São Paulo apresentando taxa de 16,6. Para efeitos de comparação a taxa em anos em torno de 1997 foi de 144,5 nos EUA, 54,4 no Canadá, 90,0 na Austrália e 31,5 em Portugal. A taxa de mortalidade no período foi de 7,2 % (EUA, 2,8%; Canadá, 2,5%: França, 3,2%). A maioria de pacientes operados foi do sexo masculino (67,5%) e a idade média foi de 59,9 anos.

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Isotopic fractionation due to sputtering has been investigated via a collector type experiment in which targets of known isotopic composition have been bombarded with several keV Ar+ and Xe+ ions with fluences down to 3.0x1014 ions/cm2 , believed to be the lowest fluences for which such detailed measurements have ever been made. The isotopes were sputtered onto carbon collectors and analyzed with Secondary Ion Mass Spectroscopy (SIMS.) There is clear indication of preferential effects several times that predicted by the dominant analytical theory. Results also show a fairly strong angular variation in the fractionation. The maximum effect is usually seen in the near normal direction, measured from the target surface, falling continuously, by a few percent in some cases, to a minimum in the oblique direction. Measurements have been made using Mo isotopes: 100Mo and 92Mo and a liquid metal system of In:Ga eutectic. The light isotope of Mo is found to suffer a 53 ± 5‰ (note: 1.0‰ ≡ 0.1%) enrichment in the sputtered flux in the near normal direction, compared to the steady state near normal sputtered composition, under 5.0 keV Xe+ bombardment of 3.0 x 1014 ions/cm2. In the liquid metal study only the angular dependence of the fractionation could be measured due to the lack of a well defined reference and the nature of the liquid surface, which is able to 'repair' itself during the course of a bombardment. The results show that 113In is preferentially sputtered over 115In in the near normal direction by about 8.7 ± 2.7‰ compared to the oblique direction. 69Ga, on the other hand, is sputtered preferentially over 71Ga in the oblique direction by about 13 ± 4.4‰ with respect to the near normal direction.

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The intensities and relative abundances of galactic cosmic ray protons and antiprotons have been measured with the Isotope Matter Antimatter Experiment (IMAX), a balloon-borne magnet spectrometer. The IMAX payload had a successful flight from Lynn Lake, Manitoba, Canada on July 16, 1992. Particles detected by IMAX were identified by mass and charge via the Cherenkov-Rigidity and TOP-Rigidity techniques, with measured rms mass resolution ≤0.2 amu for Z=1 particles.

Cosmic ray antiprotons are of interest because they can be produced by the interactions of high energy protons and heavier nuclei with the interstellar medium as well as by more exotic sources. Previous cosmic ray antiproton experiments have reported an excess of antiprotons over that expected solely from cosmic ray interactions.

Analysis of the flight data has yielded 124405 protons and 3 antiprotons in the energy range 0.19-0.97 GeV at the instrument, 140617 protons and 8 antiprotons in the energy range 0.97-2.58 GeV, and 22524 protons and 5 antiprotons in the energy range 2.58-3.08 GeV. These measurements are a statistical improvement over previous antiproton measurements, and they demonstrate improved separation of antiprotons from the more abundant fluxes of protons, electrons, and other cosmic ray species.

When these results are corrected for instrumental and atmospheric background and losses, the ratios at the top of the atmosphere are p/p=3.21(+3.49, -1.97)x10^(-5) in the energy range 0.25-1.00 GeV, p/p=5.38(+3.48, -2.45) x10^(-5) in the energy range 1.00-2.61 GeV, and p/p=2.05(+1.79, -1.15) x10^(-4) in the energy range 2.61-3.11 GeV. The corresponding antiproton intensities, also corrected to the top of the atmosphere, are 2.3(+2.5, -1.4) x10^(-2) (m^2 s sr GeV)^(-1), 2.1(+1.4, -1.0) x10^(-2) (m^2 s sr GeV)^(-1), and 4.3(+3.7, -2.4) x10^(-2) (m^2 s sr GeV)^(-1) for the same energy ranges.

The IMAX antiproton fluxes and antiproton/proton ratios are compared with recent Standard Leaky Box Model (SLBM) calculations of the cosmic ray antiproton abundance. According to this model, cosmic ray antiprotons are secondary cosmic rays arising solely from the interaction of high energy cosmic rays with the interstellar medium. The effects of solar modulation of protons and antiprotons are also calculated, showing that the antiproton/proton ratio can vary by as much as an order of magnitude over the solar cycle. When solar modulation is taken into account, the IMAX antiproton measurements are found to be consistent with the most recent calculations of the SLBM. No evidence is found in the IMAX data for excess antiprotons arising from the decay of galactic dark matter, which had been suggested as an interpretation of earlier measurements. Furthermore, the consistency of the current results with the SLBM calculations suggests that the mean antiproton lifetime is at least as large as the cosmic ray storage time in the galaxy (~10^7 yr, based on measurements of cosmic ray ^(10)Be). Recent measurements by two other experiments are consistent with this interpretation of the IMAX antiproton results.

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The temperature dependences of the reduction potentials (Eo') of wildtype human myoglobin (Mb) and three site-directed mutants have been measured by using thin-layer spectroelectrochemistry. Residue Val68, which is in van der Waals contact with the heme in Mb, has been replaced by Glu, Asp, and Asn. At pH 7.0, reduction of the heme iron (III) in the former two proteins is accompanied by uptake of a proton by the protein. The changes in Eo', and the standard entropy (ΔSo') and enthalpy (ΔHo') of reduction in the mutant proteins were determined relative to values for wild-type; the change in Eo' at 25°C was about -200 millivolts for the Glu and Asp mutants, and about -80 millivolts for the Asn mutant. Reduction of Fe(III) to Fe(II) in the Glu and Asp mutants is accompanied by uptake of a proton. These studies demonstrate that Mb can tolerate substitution of a buried hydrophobic group by potentially charged and polar residues, and that such amino acid replacements can lead to substantial changes in the redox thermodynamics of the protein.

Through analysis of the temperature dependence and shapes of NMR dispersion signals, it is determined that a water molecule is bound to the sixth coordination site of the ferric heme in the Val68Asp and in the Val68Asn recombinant proteins while the carboxyl group of the sidechain of Glu68 occupies this position in Val68Glu. The relative rhombic distortions in the ESR spectra of these mutant proteins combined with H217O and spin interconversion experiments performed on them confirm the conclusions of the NMRD study.

The rates of intramolecular electron transfer (ET) of (NH3)5Ru-His48 (Val68Asp, His81GIn, Cys110AIa)Mb and (NH3)5Ru-His48 (Val68GIu,His81GIn,Cys110Ala)Mb were measured to be .85(3)s-1 and .30(2)s-1, respectively. This data supports the hypothesis that entropy of 111 reduction and reorganization energy of ET are inversely related. The rates of forward and reverse ET for (NH3)5 Ru-His48 (Val68GIu, His81 GIn, Cys110AIa)ZnMb -7.2(5)•104s-1and 1.4(2)•105s-1, respectively- demonstrate that the placement of a highly polar residue nearby does not significantly change the reorganization energy of the photoactive Zn porphyrin.

The distal histidine imidazoles of (NH3)4isnRu-His48 SWMb and (NH3)5Ru-His48 SWMb were cyanated with BrCN. The intramolecular ET rates of these BrCN-modified Mb derivatives are 5.5(6)s-1 and 3.2(5)s-1, respectively. These respective rates are 20 and 10 times faster than those of their noncyanated counterparts after the differences in ET rate from driving force are scaled according to the Marcus equation. This increase in ET rate of the cyanated Mb derivatives is attributed to lower reorganization energy since the cyanated Mb heme is pentacoordinate in both oxidation states; whereas, the native Mb heme loses a water molecule upon reduction so that it changes from six to five coordinate. The reorganization energy from Fe-OH2 dissociation is estimated to be .2eV. This conclusion is used to reconcile data from previous experiments in our lab. ET in photoactive porphyrin-substituted myoglobins proceed faster than predicted by Marcus Theory when it is assumed that the only difference in ET parameters between photoactive porphyrins and native heme systems is driving force. However, the data can be consistently fit to Marcus Theory if one corrects for the smaller reorganization in the photoactive porphyrin systems since they do not undergo a coordination change upon ET.

Finally, the intramolecular ET rate of (NH3)4isnRu-His48 SWMb was measured to be 3.0(4)s-1. This rate is within experimental error of that for (NH3)4pyrRu-His48 SWMb even though the former has 80mV more driving force. One likely possibility for this observation is that the tetraamminepyridineruthenium group undergoes less reorganization upon ET than the tetraammineisonicotinamideruthenium group. Moreover, analysis of the (NH3)4isnRu-His48 SWMb experimental system gives a likely explanation of why ET was not observed previously in (NH3)4isnRu-Cytochrome C.

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The reaction 32S(3He, α) 31S has been used to locate 42 levels in 31S. For 11 of the first 17 levels ℓn-values have been determined. The first 6 excited states of 31S have been studied by applying the particle-gamma correlation method of Litherland and Ferguson (their Method II) to the reaction 32S(3He, αγ) 31S. The resulting spins and parities are: EX, Jπ = 1.25 MeV, 3/2+; 2.23 MeV, 5/2+; 3.08 MeV, 1/2+; 3.29 MeV, 5/2+, 3/2+; 3.35 MeV, 7/2, 3/2; 3.44 MeV, 3/2+. Mixing and branching ratios have also been determined. The ground state Q-value for the reaction 32S(3He, α)31S has been measured to be 5.538 ± 0.006 MeV. Analysis of the spectra of the reaction 32S(3He, α)33Cl which were obtained as a by-product of the spectra of the reaction 32S(3He, α) 31S located levels in 33Cl at the following excitation energies: 0, 810 ± 9, (1978 ± 14), 2351 ± 9, 2686 ± 8, 2848 ± 9 (a known doublet), 2980 ± 9, and 4119 ± 10 keV. The 2.0 MeV level was only weakly populated, and to confirm its existence the reaction 36Ar(p, α)33Cl has been studied. In this reaction the 2.0 MeV level was strongly populated and the measured excitation energy was 1999 ± 20 keV. The experimental results for 31S and 33Cl are compared with their analogs and with nuclear model predictions.

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Se cultivaron tres cepas de la división Chlorophyta (Nephroselmis pyriformis cepa CGA7, Pyramimonas orientalis cepa CGA13 y Pyramimonas propulsa cepa CGA16) en medios a cuatro pH diferentes (rango desde un control a pH 8.1 a pH7.2). Se midieron las tasas de crecimiento para cada cepa y tratamiento. Las cepas no mostraron una respuesta uniforme a la acidificación del medio, aunque todas mostraron un incremento de sus tasas de crecimiento a pH 7.5. Únicamente N. pyriformis mostró un incremento de sus tasas de crecimiento a pH 7.2. Se concluye que la división Chlorophyta no muestra una respuesta uniforme a la acidificación del medio, pero que las tasas de crecimiento pueden verse incrementadas para las especies testadas en futuros escenarios de acidificación de los océanos.

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Ce3+ and B2O3 are introduced into erbium-doped Bi2O3-SiO2 glass to enhance the luminescence emission and optic spectra characters of Er3+. The energy transfer from Er3+ to Ce3+ will obviously be improved with the phonon energy increasing by the addition of B2O3. Here, the nonradiative rate, the lifetime of the I-4(11/2) -> I-4(3/2) transition, and the emission intensity and bandwidth of the 1.5 mu m luminescence with the I-4(13/2) -> I-4(5/2) transition of Er3+ are discussed in detail. The results show that the optical parameters of Er3+ in this bismuth-borate-silicate glass are nearly as good as that in tellurite glass, and the physical properties are similar to those in silicate glass. With the Judd-Ofelt and nonradiative theory analyses, the multiphonon decay and phonon-assisted energy-transfer (PAT) rates are calculated for the Er3+/Ce3+ codoped glasses. For the PAT process, an optimum value of the glass phonon energy is obtained after B2O3 is introduced into the Er3+/Ce3+ codoped bismuth-silicate glasses, and it much improves the energy-transfer rate between Er3+ I-4(11/2)-I-4(13/2) and Ce3+ F-2(5/2) -> F-2(7/2), although there is an energy mismatch. (c) 2007 Optical Society of America.

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Part I

Potassium bis-(tricyanovinyl) amine, K+N[C(CN)=C(CN)2]2-, crystallizes in the monoclinic system with the space group Cc and lattice constants, a = 13.346 ± 0.003 Å, c = 8.992 ± 0.003 Å, B = 114.42 ± 0.02°, and Z = 4. Three dimensional intensity data were collected by layers perpendicular to b* and c* axes. The crystal structure was refined by the least squares method with anisotropic temperature factor to an R value of 0.064.

The average carbon-carbon and carbon-nitrogen bond distances in –C-CΞN are 1.441 ± 0.016 Å and 1.146 ± 0.014 Å respectively. The bis-(tricyanovinyl) amine anion is approximately planar. The coordination number of the potassium ion is eight with bond distances from 2.890 Å to 3.408 Å. The bond angle C-N-C of the amine nitrogen is 132.4 ± 1.9°. Among six cyano groups in the molecule, two of them are bent by what appear to be significant amounts (5.0° and 7.2°). The remaining four are linear within the experimental error. The bending can probably be explained by molecular packing forces in the crystals.

Part II

The nuclear magnetic resonance of 81Br and 127I in aqueous solutions were studied. The cation-halide ion interactions were studied by studying the effect of the Li+, Na+, K+, Mg++, Cs+ upon the line width of the halide ions. The solvent-halide ion interactions were studied by studying the effects of methanol, acetonitrile, and acetone upon the line width of 81Br and 127I in the aqueous solutions. It was found that the viscosity plays a very important role upon the halide ions line width. There is no specific cation-halide ion interaction for those ions such as Mg++, Di+, Na+, and K+, whereas the Cs+ - halide ion interaction is strong. The effect of organic solvents upon the halide ion line width in aqueous solutions is in the order acetone ˃ acetonitrile ˃ methanol. It is suggested that halide ions do form some stable complex with the solvent molecules and the reason Cs+ can replace one of the ligands in the solvent-halide ion complex.

Part III

An unusually large isotope effect on the bridge hydrogen chemical shift of the enol form of pentanedione-2, 4(acetylacetone) and 3-methylpentanedione-2, 4 has been observed. An attempt has been made to interpret this effect. It is suggested from the deuterium isotope effect studies, temperature dependence of the bridge hydrogen chemical shift studies, IR studies in the OH, OD, and C=O stretch regions, and the HMO calculations, that there may probably be two structures for the enol form of acetylacetone. The difference between these two structures arises mainly from the electronic structure of the π-system. The relative population of these two structures at various temperatures for normal acetylacetone and at room temperature for the deuterated acetylacetone were calculated.

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Up-conversion luminescence characteristics under 975 nm excitation have been investigated with Tb3+/Tm3+/Yb3+ triply doped tellurite glasses. Here, green (547 nm: D-5(4) --> F-7(4)) and red (660 nm: D-5(4) --> F-7(2)) up-conversion (UC) luminescence originating from Tb3+ is observed strongly, because of the quadratic dependences of emission intensities on the excitation power. Especially, the UC luminescence was intensified violently with the energy transfer from the Tm3+ ions involves in the Tb3+ excitation. To the Tb3+/Tm3+/Yb3+ triply doped glass system, a novel up-conversion mechanism is proposed as follows: the energy of (3)G(4) level (Tm3+) was transferred to D-5(4) (Tb3+) and the 477-nm UC luminescence of Tm3+ was nearly quenched. (C) 2006 Elsevier B.V. All rights reserved.

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A despeito de suas limitações, os dados do SIHSUS são os mais sistemáticos e abrangentes sobre as Reações Adversas e Intoxicações a medicamentos que provocam hospitalização. Eles demonstram a importância das ações de educação e investigação de casos do Programa Nacional de Farmacovigilância para possibilitar o diagnóstico mais acurado e superação do quadro atual de ocorrência desses agravos, além da possibilidade de o SIH/SUS ser utilizado sistematicamente como fonte de dados na detecção e análise dos problemas relacionados a medicamentos. No período de 1999 a 2007, foram emitidas 6.670.609 AIH (tipo 1), entre as quais 3.611 foram classificadas como internações devidas a RAM e 4.675 como Intoxicações, correspondendo, respectivamente, às taxas médias de 5,41 casos por 104 AIH e 7,2 casos por 104 AIH. Ocorreram 137 óbitos (3,79% das AIH) por RAM e 207 (4,43% das AIH) por Intoxicações na população internada. Tanto as RAM como as Intoxicações tiveram menor chance de levar ao óbito quando comparados às outras causas. Uma característica da distribuição dos RAM foi concentrar 62% das AIH nas faixas etárias de 20 a 59 anos de idade (grupo adulto). Nas Intoxicações merece destaque a elevada proporção de AIH na faixa etária de 0-4 anos (14,29%). As AIH registradas com causas básicas relacionados a RAM foram principalmente de pacientes do sexo masculino, já as Intoxicações foram principalmente de pacientes do sexo feminino. Em ambos tipos de agravos estes pacientes foram internados em hospitais que não faziam parte da Rede de Hospitais Sentinelas do Programa Nacional de Farmacovigilância. No entanto, a probabilidade destes hospitais registrarem as AIH com códigos CID-10 referentes às RAM é maior, o que ocorre provavelmente por estarem mais capacitados em diagnosticar este tipo de agravo. Porém este fato não foi observado para as Intoxicações. Os fármacos que causaram os agravos estudados são psicoativos. Este estudo apresentou algumas evidências sobre a distribuição da morbi-mortalidade provocada por medicamentos entre pacientes internados em hospitais conveniados ao SUS no período de 1999-2007, baseadas nas informações das AIH, que podem ser úteis ao Programa de Farmacovigilância no Estado do Rio de Janeiro.