44 resultados para Aguado, Olympe (1827-1894)


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Microcrystalline silicon thin films at different growth stages were prepared by hot wire chemical vapor deposition. Atomic force microscopy has been applied to investigate the evolution of surface topography of these films. According to the fractal analysis I it was found that, the growth of Si film deposited on glass substrate is the zero-diffused stochastic deposition; while for the film on Si substrate, it is the finite diffused deposition on the initial growth stage, and transforms to the zero-diffused stochastic deposition when the film thickness reaches a certain value. The film thickness dependence of island density shows that a maximum of island density appears at the critical film thickness for both substrates. The data of Raman spectra approve that, on the glass substrate, the a-Si: H/mu c-Si:H transition is related to the critical film thickness. Different substrate materials directly affect the surface diffusion ability of radicals, resulting in the difference of growth modes on the earlier growth stage.

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综合基于角色的访问控制和信任管理各自的优势,提出了一个适用于开放式环境的细粒度可控委托授权模型--FCDAM(fine-grained controllable delegation authorization model),基于信任度实现了对角色中具有不同敏感度的权限传播控制.提出了为本地策略中的权限分配信任度阈值的方法,为RT_0添加了信任度支持,给出了在这种扩展后的信任管理系统中计算实体信任度的算法,并结合具体实例对模型的使用进行了说明.

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We present an all-e-beam lithography (EBL) process for the patterning of photonic crystal waveguides.The whole device structures are exposed in two steps. Holes constituting the photonic crystal lattice and defects are first exposed with a small exposure step size (less than 10nm). With the introduction of the additional proximity effect to compensate the original proximity effect, the shape, size, and position of the holes can be well controlled.The second step is the exposure of the access waveguides at a larger step size (about 30nm) to improve the scan speed of the EBL. The influence of write-field stitching error can be alleviated by replacing the original waveguides with tapered waveguides at the joint of adjacent write-fields. It is found experimentally that a higher exposure efficiency is achieved with a larger step size;however,a larger step size requires a higher dose.

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采用热丝化学气相沉积技术制备了一系列处于不同生长阶段的薄膜样品,用原子力显微镜系统地研究生长在单晶硅衬底和玻璃衬底上薄膜表面形貌的演化.按照分形理论分析得到:在玻璃衬底上的硅薄膜以零扩散随机生长模式生长;而在单晶硅衬底上,薄膜早期以有限扩散生长模式生长,当膜厚超过某一临界厚度时转变为零扩散随机生长模式.岛面密度与膜厚的依赖关系表明,在临界厚度时硅衬底和玻璃衬底上的岛面密度均出现了极大值.Raman谱的测量证实,玻璃衬底上薄膜临界厚度与非晶/微晶相变之间存在密切的关系.不同的衬底材料直接影响反应基元的表面扩散能力,从而造成薄膜早期生长模式的差异.

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The traditional design of accelerator magnet usually involves many time consuming iterations of the manual analysis process. A software platform to do these iterations automatically is proposed in this paper. In this platform, we use DAKOTA (a open source software developed by Sandia National Laboratories) as the optimizing routine, which provides a variety of optimization methods and algorithms, and OPERA (software from Vector Fields) is selected as the electromagnetic simulating routine. In this paper, two examples of designs of accelerator magnets are used to illustrate how an optimization algorithm is chosen and the platform works.

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A simple method was developed for injecting a sample on a cross-form microfluidic chip by means of hydrostatic pressure combined with electrokinetic forces. The hydrostatic pressure was generated simply by adjusting the liquid level in different reservoirs without any additional driven equipment such as a pump. Two dispensing strategies using a floating injection and a gated injection, coupled with hydrostatic pressure loading, were tested. The fluorescence observation verified the feasibility of hydrostatic pressure loading in the separation of a mixture of fluorescein sodium salt and fluorescein isothiocyanate. This method was proved to be effective in leading cells to a separation channel for single cell analysis.

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根据长白山阔叶红松林 2 0 0 1年 5月下旬至 10月上旬微气象梯度观测资料和辐射、土壤热通量资料 ,用波文比 -能量平衡方法 (BREB方法 )计算了森林的显热通量和感热通量 ,并计算了森林大气和植被体的储热量 ,分析了阔叶红松林热量平衡各项的日变化和季节变化 ,结果发现 ,热量平衡 (净辐射 )与太阳总辐射呈线性关系 ;热量平衡各项都与净辐射有相同的日变化特征 ,为昼正夜负的曲线 .各项的绝对值一般表现为净辐射 >潜热通量 >感热通量 >储热变化 .受日照时间的影响 ,6~ 10月各分量正值的日持续时间逐渐缩短 .月平均结果 ,白天净辐射 6月份最大 ,10月上旬最小 ,变化于 0~ 5 2 7W·m-2 ,夜间的净辐射在 0~ - 12 1W·m-2 .潜热通量白天和夜间分别在 0~ 4 4 1、0~ - 81W·m-2 ,感热通量昼夜分别在 0~80、0~ - 2 6W·m-2 .储热变化则为 0~ 4 4、0~ - 2 6W·m-2 .白天潜热通量占净辐射的比例 8~ 10月逐渐下降 ,而感热通量和储热变化的比例 9~ 10月明显上升 ,特别在严霜后 2~ 3d ,出现潜热通量比例突减、感热通量比例突增的现象 .文中还对通量观测仪器、方法进行了简要分析 .