944 resultados para spontaneous


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Neurons obtained directly from human somatic cells hold great promise for disease modeling and drug screening. Available protocols rely on overexpression of transcription factors using integrative vectors and are often slow, complex, and inefficient. We report a fast and efficient approach for generating induced neural cells (iNCs) directly from human hematopoietic cells using Sendai virus. Upon SOX2 and c-MYC expression, CD133-positive cord blood cells rapidly adopt a neuroepithelial morphology and exhibit high expansion capacity. Under defined neurogenic culture conditions, they express mature neuronal markers and fire spontaneous action potentials that can be modulated with neurotransmitters. SOX2 and c-MYC are also sufficient to convert peripheral blood mononuclear cells into iNCs. However, the conversion process is less efficient and resulting iNCs have limited expansion capacity and electrophysiological activity upon differentiation. Our study demonstrates rapid and efficient generation of iNCs from hematopoietic cells while underscoring the impact of target cells on conversion efficiency.

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为定量分析放大自发辐射(ASE)对调Q激光器性能的影响,在调Q激光速率方程中引入放大自发辐射项。并在合理的近似下求解,给出了激光二极管(LD)端面抽运电光调Q运转的固体激光器反转粒子数的建立过程,分析了放大自发辐射对激光上能级储能效率的影响及考虑放大自发辐射时调Q激光器输出脉冲宽度和脉冲能量随抽运功率的变化关系。结果表明,由于放大自发辐射的存在,上能级储能效率降低,且在一定的抽运功率下,调Q输出脉冲宽度变宽,脉冲能量下降。用LGS(La3Ga5SiO14)晶体作电光调Q元件,在激光二极管抽运的Nd:YVO

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报道了一种MOPA式国产单频光纤放大器。该放大器采用连续波单频激光器作为主振荡器,采用我国自行设计和制造的大模场面积掺Yb双包层光纤作为功率放大器,在波长1064 nm处实现了最高7.3 W的连续激光输出,斜率效率为39%,光-光转换效率为26%。此外,对光谱特性及放大的自发发射的抑制也进行了探讨。

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Alguns estudos na área da Psicolinguística tratam sobre a interrupção da forma natural da fluência da fala. Essas suspensões são denominadas disfluências e podem ser de variados tipos como, por exemplo, repetições, substituições ou pausas. Entre alguns trabalhos sobre disfluências, destaca-se o realizado por Jaeger (2005), que tratou da omissão do relativizador that na língua inglesa e a possibilidade desse fator ser responsável pela criação de disfluências. Nessa mesma linha, objetivamos analisar as disfluências na camada dos relativizadores camada CP em língua portuguesa brasileira. Para isso, tomaram-se dados obtidos por Corrêa et al (2008) sobre produção de orações relativas. Nesse estudo, os autores, buscando verificar a complexidade da formulação de orações relativas, manipularam duas condições: plenamente planejada que reduziria a carga de processamento e, consequentemente, levaria à maior produção de orações relativas padrões e parcialmente planejada a qual aumentaria a carga de processamento e, consequentemente, maior produção de orações relativas cortadoras e resumptivas. Diante disso, sabendo que o planejamento de estruturas mais complexas pode ser um fator que gere mais sentenças disfluentes, resta saber em qual das condições, estipuladas por Corrêa et al (2008), haveria maior caso de disfluências. Acreditamos que a condição parcialmente planejada resultaria mais casos de disfluências em comparação à condição inteiramente planejada. Para verificação de tal hipótese, a presente pesquisa focou suas atenções no banco de dados de Corrêa et al (2008). Após determinados critérios, privilegiamos sentenças de orações relativas genitivas, orações relativas de objeto indireto funcional e orações relativas de objeto indireto lexical, pois tais seriam construções sintáticas mais complexas e passíveis de terem mais casos de disfluências. Identificadas e quantificadas todas as falas de interesse, criamos tabelas para melhor visualização das disfluências em localizações específicas na sentença como, por exemplo, antes da oração relativa (AOR), na oração relativa (NAOR) e depois da oração relativa (DPOR). Com tais dados analisados, verificamos que eles corroboravam a hipótese levantada: na condição parcialmente planejada há mais casos de disfluências do que na condição inteiramente planejada, principalmente quando se é focalizada a localização NAOR. Entre os principais resultados, percebemos que as disfluências do tipo pausas preenchidas aparecem em grande quantidade na localização NAOR, fator que revela uma característica especial da oração relativa. Essa disfluência, nesse trecho da sentença, revela que os falantes não somente fazem uma procura lexical, como também, um planejamento discursivo. Tais resultados nos motivaram a pensar em outras determinadas situações de pesquisa como, por exemplo, a análise das disfluências em sentenças de voz passiva

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制备了四种不同铒离子掺杂浓度的碲酸盐玻璃,通过测定吸收光谱计算了吸收谱线的振子强度,根据Judd-Ofelt理论计算了不同浓度下Er^3+离子发光光谱的强度参数Ω(i=2,4,6),计算了自发辐射电偶和磁偶跃迁概率、辐射寿命、荧光分支比等参数,讨论了Er^3+离子浓度变化对以上这些参数的影响。测试了Er^3+:^4I13/2→^4I15/2跃迁对应的荧光光谱和Er^3+:^4I13/2能级荧光寿命。最后应用McCumber理论计算了玻璃中Er^3+:^4I13/2→^4I15/2跃迁对应的受激发射截面大小

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The integrated absorption cross section Sigma(abs), I peak emission cross section sigma(cmi), Judd-Ofeld intensity parameters Omega(iota) ( t = 2,4,6), and spontaneous emission probability A(R) of Er3+ ions were determined for Erbium doped alkali and alkaline earth phosphate glasses. It is found the compositional dependence of sigma(emi) 5 almost similar to that of Sigma(abs), which is determined by the sum, of Omega(1) (3 Omega(2) + 10 Omega(4) + 21 Omega(6)). In addition, the compositional dependence of Omega(1) was studied in these glass systems. As a result, compared with. Omega(4) and Omega(6) the Omega(2) has a stronger compositional dependence on the ionic radius and content of modifers. The covalency of Er-O bonds in phosphate glass is weaker than that in silicate glass, germanate glass, aluminate glass, and tellurate glass, since Omega(6) of phosphate glass is relatively large. A(R) is affected by the covalency of the Er3+ ion sites and corresponds to the Omega(6) value.

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Er3+-doped lithium-potassium mixed alkali aluminophosphate glasses belonging to the oxide system xK(2)O-(15x)Li2O-4B(2)O(3)-11Al(2)O(3)-5BaO-65P(2)O(5) are obtained in a semi-continuous melting quenching process. Spectroscopic properties of Er3+-doped glass matrix have been analysed by fitting the experimental data with the standard Judd-Ofelt theory. It is observed that Judd-Ofelt intensity parameters-Omega(t)(t=2, 4 and 6) of Er3+ change when the second alkali is introduced into glass matrix. The variation of line strength S-ed[I-4(13/2),I-4(15/2)] follows the same trend as that of the Omega(6) parameter. The effect of mixed alkali on the spectroscopic properties of the aluminophosphate glasses, such as absorption cross-section, stimulated emission cross-section, spontaneous emission probability, branching ratio and the radiative lifetime, has also been investigated in this paper.

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Dy3+ doped oxyfluoride silicate glass was prepared and its optical absorption, 1.3 mu m emission, and upconversion luminescence properties were studied. Furthermore, the Judd-Ofelt [Phys. Rev. 127, 750 (1962); J. Chem. Phys. 37, 511 (1962)] intensity parameters, oscillator strengths, spontaneous transition probability, fluorescence branching ratio and radiative lifetime were calculated by Judd-Ofelt theory, while stimulated emission cross section of H-6(9/2)+F-6(11/2)-> H-6(15/2) transition was calculated by McCumber theory [Phys. Rev. A. 134, 299 (1964)]. According to the obtained Judd-Ofelt intensity parameters Omega(2)=2.69x10(-20) cm(2), Omega(4)=1.64x10(-20) cm(2), and Omega(6)=1.64x10(-20) cm(2), the radiative lifetime was calculated to be 810 mu s for 1.3 mu m emission, whose full width at half maximum and sigma(e) were 115 nm and 2.21x10(-20)cm(2), respectively. In addition, near infrared to visible upconversion luminescence was observed and evaluated. The results suggest that Dy3+ doped oxyfluoride silicate glass can be used as potential host material for developing broadband optical amplifiers and laser applications.

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The Er3+/Yb3+ co-doped glasses with compositions of xBi(2)O(3)-(65-x)P2O5-4Yb(2)O(3)-11Al(2)O(3)-5BaO-15Na(2)O (where x = 0, 2.5, 5, 7.5 and 10 mol%) were prepared using the normal melt quench technique. The optical absorption spectra of the glasses were recorded in the wavelength range 300-1700 nm. The effect of Bi2O3 content on the thermal stability and absorption spectra of glasses was investigated. In addition, the Judd-Ofelt parameters and oscillator strengths were calculated by employing Judd-Ofelt theory. It was observed that the positions of the fundamental absorption edge and cut-off wavelength shifted towards red as the content of Bi2O3 increased. However, there were no red shifts found both in the peak wavelength and in the center of mass wavelength of all absorption bands with Bi2O3 content increasing. The results of Judd-Ofelt theory analysis showed that Judd-Ofelt parameters Omega(t), (t = 2, 4, 6) changed sharply when Bi2O3 concentration exceeded 5 mol%. The variation trends of experimental oscillator strength were similar with those of Judd-Ofelt parameters as function of Bi2O3 concentrations. Moreover, differential scanning calorimetry experiments showed that the increases of Bi2O3 content weakened the network structure and then lowered the thermal stability of the glasses. The spontaneous emission probability A(rad), branching ratio beta and the radiative lifetime tau(rad) were also calculated and analyzed. The stimulated emission cross-section of Er3+ was calculated according to the McCumber theory. It was found that the stimulated emission cross-section of Er3+ was monotonically increases with Bi2O3 content increasing. (C) 2006 Elsevier B.V. All rights reserved.

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The thermal stability, 2 μm fluorescence properties and energy transfer mechanism in Ho3+ doped fluorophosphate glass sensitized by Yb3+ and Tm3+ were investigated. The characteristic temperatures, absorption spectrum and fluorescence spectrum of the glass sample were measured. ΔT calculated from the characteristic temperatures shows that the thermal stability of fluorophosphate glass is better than fluoride glass. According to the absorption spectrum, several spectroscopic parameters of the glass sample, such as Judd-Ofelt parameters and spontaneous transition probability were calculated and compared with other glass hosts. The largest spontaneous transition probability for Ho3+:5 I7&rarr5I8 transition in fluorophosphate glass which is 78.48 s-1 indicates that fluorophosphate glass is an appropriate base glass to achieve 2 m fluorescence. From the fluorescence spectrum of the glass sample, the extremely strong 2.0 μm fluorescence intensity is observed, which is higher than the intensity of 1.8 μm fluorescence, showing that Ho3+ ions sensitized by Yb3+ and Tm3+ is efficient. Meanwhile, the absorption sections and emission sections of Yb3+, Tm3+ and Ho3+ were calculated and the pumping scheme and energy transfer mechanism among Yb3+, Tm3+ and Ho3+ are discussed. The study indicates that Yb-Tm-Ho tri-doped fluorophosphate glass is a significant sensitization glass system under 980 nm excitation for 2 μm applications.

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2.0 μm spectroscopic properties of Er3+/Tm3+/Ho3+ triply-doped fluorophosphate glasses pumped by 808 nm and the energy transfer mechanisms between the three rare earth ions were investigated. J-O theory was used to calculate the parameters of Ho3+ in fluorophosphate glasses. Absorption and emission cross-sections and the gain coefficients were calculated. The obtained lifetime r and spontaneous transition probability Ar of Ho3+:5I7 level were 10.64 ms and 93.95 s-1 respectively. The calculated maximum emission cross-section of 2.0 μm was 9.26×10-21 cm2. The energy transfer analysis indicated that the cross-relaxation of Tm3+ was important and the resonent energy transfer in Er3+&rarrHo3+, Tm3+&rarrHo3+, Er3+&rarrTm3+&rarrHo3+ process was the main channel. The study revealed that the Er3+/Tm3+/Ho3+ triply-doped fluorophosphate glass would be a potential material for 2.0 μm emission because of the efficient sensitization of Er3+ and Tm3+ to Ho3+.

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Er3+-doped TeO2-based oxysulfide glasses have been prepared in argon atmosphere in carbon crucibles. The thermal analysis and spectroscopic properties of Er (3+) have been considered in terms of sulfide influence. As a function of composition, we have principally measured optical absorption, spontaneous emission and lifetime measurements. Judd-Ofelt theory was introduced to calculate bandwidth and emission cross-section. The results show the product FVMM x sigma(c) increase from 476.8 8 to 635.04 10(-21) cm(2) nm evidently with the addition of 10 mol% PbS into tellurite glass, which indicates a perfect effect on spectra property of Er3+ ions. (C) 2004 Elsevier B.V. All rights reserved.

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Tellurite glass is proposed as a host for broadband erbium-doped fiber amplifiers because of their excellent optical and chemical properties. A new single mode Er3+/Yb3+ codoped tellurite fiber with D-shape cladding geometry is fabricated in this work. When pumped at 980 nm, a broad erbium amplified spontaneous emission (ASE) nearly 100 nm in the wavelength range of 1450-1650 ran around 1.53 mu m is observed. It was found that the emission spectrum from erbium in tellurite glass fibers is almost twice as broad as the corresponding spectrum in tellurite bulk glass. The changes in ASE with regard to fiber lengths and pumping power were measured and discussed. The output of about 2.3 mW from Er3+/Yb3+ codoped tellurite fiber ASE source is obtained under the pump power of 700 mW. The broad 1.53 mu m emission of Er3+ in Er3+/Yb3+ codoped tellurite glass fiber can be used as host material for potential broadband optical amplifier and tunable fiber lasers. (c) 2005 Elsevier B.V. All rights reserved.

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测试了不同掺杂浓度和样品厚度下掺铒磷酸盐和碲酸盐玻璃的吸收光谱、荧光光谱和荧光寿命,计算了Er^3+离子在1.53μm处的吸收截面(σa)、发射截面(σe)、自发辐射跃迁概率(Arad)、辐射跃迁寿命(τrad)、以及辐射跃迁量子效率(η)等光谱参数.讨论了荧光俘获效应对掺铒磷酸盐和碲酸盐玻璃光谱性质及光谱参数的影响.结果表明即使在铒离子低掺杂浓度(0.1mol%Er2O3)下,荧光俘获效应也普遍存在于掺铒玻璃材料中,使得荧光寿命(τt)和荧光半高宽(FWHM)随样品的厚度和铒离子掺杂浓度增加而增大,导致

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A comprehensive study on the thermal stability and spectroscopic properties of Er3+/Yb3+-codoped Al(PO3)(3)-based fluorophosphate glasses is reported of the 1.5μ m fibre amplifiers in this paper. From optical absorption spectra, the Judd-Ofelt parameters of Er3+ in the glasses and several important optical properties, such as the radiative transition probability, the branching ratio and the spontaneous emission probability, have been calculated by using Judd-Ofelt theory. The fluorophosphate glass exhibits broadband near-infrared emission at 1.53μ m with a full width at half-maximum over 63nm, and a large calculated stimulated-emission cross-section of 6.85 x 10(-21)cm(2).