997 resultados para diffraction efficiency spectrum


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Of 33 phages isolated from various shrimp farms in Kerala, India, six were segregated to have broad spectrum lytic efficiency towards 87 isolates of Vibrio harveyi with cross-infecting potential to a few other important aquaculture pathogens. They were further tested on beneficial aquaculture micro-organisms such as probiotics and nitrifying bacterial consortia and proved to be noninfective. Morphological characterization by transmission electron microscopy (TEM) and molecular characterization by RAPD and SDS-PAGE proved them distinct and positioned under Caudovirales belonging to Myoviridae and Siphoviridae

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Gallaborane (GaBH6, 1), synthesized by the metathesis of LiBH4 with [H2GaCl]n at ca. 250 K, has been characterized by chemical analysis and by its IR and 1H and 11B NMR spectra. The IR spectrum of the vapor at low pressure implies the presence of only one species, viz. H2Ga(μ-H)2BH2, with a diborane-like structure conforming to C2v symmetry. The structure of this molecule has been determined by gas-phase electron diffraction (GED) measurements afforced by the results of ab initio molecular orbital calculations. Hence the principal distances (rα in Å) and angles ( α in deg) are as follows: r(Ga•••B), 2.197(3); r(Ga−Ht), 1.555(6); r(Ga−Hb), 1.800(6); r(B−Ht), 1.189(7); r(B−Hb), 1.286(7); Hb−Ga−Hb, 71.6(4); and Hb−B−Hb, 110.0(5) (t = terminal, b = bridging). Aggregation of the molecules occurs in the condensed phases. X-ray crystallographic studies of a single crystal at 110 K reveal a polymeric network with helical chains made up of alternating pseudotetrahedral GaH4 and BH4 units linked through single hydrogen bridges; the average Ga•••B distance is now 2.473(7) Å. The compound decomposes in the condensed phases at temperatures exceeding ca. 240 K with the formation of elemental Ga and H2 and B2H6. The reactions with NH3, Me3N, and Me3P are also described.

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Carbon tetrafluoride (CF4) is included as a greenhouse gas within the Kyoto Protocol. There are significant discrepancies in the reported integrated infrared (IR) absorption cross section of CF4 leading to uncertainty in its contribution to climate change. To reduce this uncertainty, the IR spectrum of CF4 was measured in two different laboratories, in 0 933 hPa of air diluent at 296 +/- 2K over the wavelength range 600-3700 cm(-1) using spectral resolutions of 0.03 or 0.50 cm(-1). There was no discernable effect of diluent gas pressure or spectral resolution on the integrated IR absorption, and a value of the integrated absorption cross section of (1.90 +/- 0.17) x 10(-16) cm(2) molecule(-1) cm(-1) was derived. The radiative efficiency (radiative forcing per ppbv) and GWP (relative to CO2) of CF4 were calculated to be 0.102 W m(-2) ppbv(-1) and 7200 (100 year time horizon). The GWP for CF4 calculated herein is approximately 30% greater than that given by the Intergovernmental Panel on Climate Change (IPCC) [ 2002] partly due to what we believe to be an erroneously low value for the IR absorption strength of CF4 assumed in the calculations adopted by the IPCC. The radiative efficiency of CF4 is predicted to decrease by up to 40% as the CF4 forcing starts to saturate and overlapping absorption by CH4, H2O, and N2O in the atmosphere increases over the period 1750-2100. The radiative forcing attributable to increased CF4 levels in the atmosphere from 1750 to 2000 is estimated to be 0.004 W m(-2) and is predicted to be up to 0.033 W m(-2) from 2000 to 2100, dependent on the scenario.

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Context: Inherited GH insensitivity (GHI) is usually caused by mutations in the GH receptor (GHR). Patients present with short stature associated with high GH and low IGF-I levels and may have midfacial hypoplasia ( typical Laron syndrome facial features). We previously described four mildly affected GHI patients with an intronic mutation in the GHR gene (A.(1) -> G.(1) substitution in intron 6), resulting in the activation of a pseudoexon (6 Psi) and inclusion of 36 amino acids. Objective: The study aimed to analyze the clinical and genetic characteristics of additional GHI patients with the pseudoexon (6 Psi) mutation. Design/Patients: Auxological, biochemical, genetic, and haplotype data from seven patients with severe short stature and biochemical evidence of GHI were assessed. Main Outcome Measures: We assessed genotype-phenotype relationship. Results: One patient belongs to the same extended family, previously reported. She has normal facial features, and her IGF-I levels are in the low-normal range for age. The six unrelated patients, four of whom have typical Laron syndrome facial features, have heights ranging from -3.3 to -6.0 SD and IGF-I levels that vary from normal to undetectable. We hypothesize that the marked difference in biochemical and clinical phenotypes might be caused by variations in the splicing efficiency of the pseudoexon. Conclusions: Activation of the pseudoexon in the GHR gene can lead to a variety of GHI phenotypes. Therefore, screening for the presence of this mutation should be performed in all GHI patients without mutations in the coding exons.

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Nickel cyanide is a layered material showing markedly anisotropic behaviour. High-pressure neutron diffraction measurements show that at pressures up to 20.1 kbar, compressibility is much higher in the direction perpendicular to the layers, c, than in the plane of the strongly chemically bonded metal-cyanide sheets. Detailed examination of the behaviour of the tetragonal lattice parameters, a and c, as a function of pressure reveal regions in which large changes in slope occur, for example, in c(P) at 1 kbar. The experimental pressure dependence of the volume data is fitted to a bulk modulus, B0, of 1050 (20) kbar over the pressure range 0–1 kbar, and to 124 (2) kbar over the range 1–20.1 kbar. Raman spectroscopy measurements yield additional information on how the structure and bonding in the Ni(CN)2 layers change with pressure and show that a phase change occurs at about 1 kbar. The new high-pressure phase, (Phase PII), has ordered cyanide groups with sheets of D4h symmetry containing Ni(CN)4 and Ni(NC)4 groups. The Raman spectrum of phase PII closely resembles that of the related layered compound, Cu1/2Ni1/2(CN)2, which has previously been shown to contain ordered C≡N groups. The phase change, PI to PII, is also observed in inelastic neutron scattering studies which show significant changes occurring in the phonon spectra as the pressure is raised from 0.3 to 1.5 kbar. These changes reflect the large reduction in the interlayer spacing which occurs as Phase PI transforms to Phase PII and the consequent increase in difficulty for out-of-plane atomic motions. Unlike other cyanide materials e.g. Zn(CN)2 and Ag3Co(CN)6, which show an amorphization and/or a decomposition at much lower pressures (~100 kbar), Ni(CN)2 can be recovered after pressurising to 200 kbar, albeit in a more ordered form.

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Fundação de Amparo à Pesquisa do Estado de São Paulo (FAPESP)

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Fundação de Amparo à Pesquisa do Estado de São Paulo (FAPESP)

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Fundação de Amparo à Pesquisa do Estado de São Paulo (FAPESP)

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Fundação de Amparo à Pesquisa do Estado de São Paulo (FAPESP)

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Ultrafast photoinduced absorption by IRAV modes is used to detect charged solitons in oriented polyacetylene. We find that soliton pairs are photogenerated within our time resolution of similar to250 fs with similar to100% quantum efficiency (phi(ch)). The excitation spectrum of phi(ch) shows an onset at 1.0 eV, with a weak photon energy dependence up to 4.7 eV. These results agree with the ultrafast soliton formation predicted by Su and Schrieffer and with the SSH threshold of 2E(g)/pi for soliton pair production.

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The present study suggests the use of high energy ball milling to mix (to dope) the phase MgB2 with the AlB2 crystalline structure compound, ZrB2, with the same C32 hexagonal structure than MgB 2, in different concentrations, enabling the maintenance of the crystalline phase structures practically unaffected and the efficient mixture with the dopant. The high energy ball milling was performed with different ball-to-powder ratios. The analysis of the transformation and formation of phases was accomplished by X-ray diffractometry (XRD), using the Rietveld method, and scanning electron microscopy. As the high energy ball milling reduced the crystallinity of the milled compounds, also reducing the size of the particles, the XRD analysis were influenced, and they could be used as comparative and control method of the milling. Aiming the recovery of crystallinity, homogenization and final phase formation, heat treatments were performed, enabling that crystalline phases, changed during milling, could be obtained again in the final product. © (2010) Trans Tech Publications.

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O presente trabalho visa investigar o Processo de Craqueamento Termocatalítico do Óleo de Buriti (Mauritia flexuosa L.), óleo de palma (Elaeis guineensis) e sabão de óleo de buriti, considerando a transformação dos óleos vegetais e sabões via craqueamento termocatalítico em biocombustíveis, utilizando-se Na2CO3 (Carbonato de Sódio), CaCO3 (Carbonato de Cálcio),CaO (óxido de cálcio) e Zeólitas Ácidas (HZSM-5) como catalisadores,as temperaturas de 420, 450 e 480 °C.O fruto de Buriti (Mauritia flexuosa L.) foi coletado e extraído óleo da polpa, em seguida este óleo foi caracterizado em relação Índice de Acidez, Índice de saponificação, Viscosidade Cinemática, Densidade , Índice de Refração e análise de CHN.Para testes preliminares foi utilizado o óleo de palma refinado e neutralizado portanto eles não foram caracterizados.O sabão de buriti foi preparado em laboratório com hidróxido de potássio e hidróxido de sódio e armazenados para pirólise térmica.Os catalisadores também foram caracterizados com relação ao infravermelho,Ressonância Magnética Nuclear de 29Si e 27Al, difração de raio X ,análise térmica, análise química e TPD de Amônia .No processo de craqueamento termocatalítico os produtos líquidos produzidos foram analisados quanto aos parâmetros: rendimento, índice de acidez, espectro de infravermelho, espectro de RMN e análise de CHN em seguida foram caracterizados com relação à densidade e viscosidade cinemática. No entanto, com relação ao índice de acidez dos produtos líquidos, somente os catalisadores básicos produziram craqueados com valores aceitáveis para utilização como combustível. A partir dos resultados verificou-se a eficiência dos catalisadores no qual o catalisador carbonato de sódio forneceu produtos de baixa acidez e com boas características para uso como combustível.

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Neste trabalho, cristais de sulfato níquel dopados com íons de manganês (NSH: Mn) e cristais de sulfato níquel dopados com de íon de magnésio (NMgSH) foram crescidos e posteriormente caracterizados pelas técnicas de difração de raios X e de espectroscopia Raman. Os resultados obtidos mostraram que os cristais dopados possuem estrutura muito semelhante a do cristal de sulfato de níquel puro (NSH), com uma deformação anisotrópica nas dimensões da célula unitária em relação ao cristal puro. O objetivo do presente estudo foi crescer dois novos monocristais de boa qualidade óptica para serem usados como filtros ópticos de banda passante. Os cristais de sulfato de níquel hexa-hidratado (NHS) são conhecidos por possuírem espectros de transmissão óptica, que tem atraído muita atenção, pois apresentam duas regiões com alta eficiência de transmissão, aproximadamente 80%, sendo a primeira região entre 200 e 350 nm e a segunda entre 400 e 600 nm, e uma alta eficiência de absorção em outras regiões do espectro UV-VIS. Um espectro de transmissão de luz com estas características é semelhante a um filtro óptico. Analises Termogravimetric (TGA) foram realizadas para cristais puros e dopados. A temperatura de decomposição obtida para o NSH foi de 73 ° C, enquanto que os cristais de NSH:Mn e NMgSH apresentam valores de 82 ° C e 86 º C, respectivamente. Como pode ser facilmente percebido, a estabilidade térmica de cristais com o íons de Mn ou Mg em suas estruturas é significativamente maior. A banda de transmissão entre 200 e 350 nm no espectro óptico de NSH foi observada com redução significativa em sua largura nos espectros de transmissão dos cristais dopados restringindo assim a região do espectro conhecida como UVA.