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Development of a New Cluster Beam Source for the Vacuum Synthesis of Nanostructures (2)

机译:开发用于真空合成纳米结构的新型簇束源(2)

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We observed the images of the vapor front directly in the confinement processes. A pulsed Nd:YAG laser (wave length 532nm, pulse duration 10ns, energy 50mJ/ pulse) is introduced via a plate set for shock waves reflected, and irradiates a silicon target mounted at 23mm far from the plate. We carefully poured the helium gas with no turbulent flow into the cluster generation cell along the spherical surface of the target holder. A bright image of photo-emission from the vapor front in the sufficient helium ambient was observed at the position of 6mm far from the target by using a high-speed image intensifier (Fig.5a). The image of the front edge is so much sharp as 0.4mm in boundary, compared to that in the condition of lower helium pressure (Fig.5b). This fact means that the density of vapor particles in the front edge is reduced with a steep gradient at the boundary, and the confinement of the mixed gas layer is achieved in a narrow space in 0.4mm.
机译:我们在封闭过程中直接观察到了蒸气前沿的图像。脉冲Nd:YAG激光(波长532nm,脉冲持续时间10ns,能量50mJ /脉冲)通过一个板组引入,用于反射的冲击波,并照射远离板的23mm处安装的硅靶。我们小心地将没有湍流的氦气沿靶支架的球形表面倒入簇生成池中。通过使用高速图像增强器,在距目标6mm的位置,在足够的氦气环境中观察到了从蒸气前沿发出的光致发光图像(图5a)。与较低氦气条件下的图像相比,前边缘的图像边界清晰至0.4mm(图5b)。该事实意味着,在边界处,蒸气颗粒的密度以陡峭的梯度减小,并且在0.4mm的狭窄空间中实现了混合气体层的限制。

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