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Space‐resolved extreme ultraviolet emission from laser‐produced plasmas

机译:空间连字符;激光连字符产生的等离子体的极紫外发射

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We have obtained extreme ultraviolet (XUV) spectra of plasmas created by focusing nanosecond CO2laser pulses onto massive planar targets of Al, Ti, and CH2. The instrument used to obtain these spectra was a normal incidence extreme ultraviolet spectrograph with the entrance slit removed. The concave spherical grating of such a slitless spectrograph diffracts and focuses the XUV radiation, and the resulting images are recorded on Kodak 101 film. The XUV images are therefore space resolved but time averaged over the lifetime of the plasma. The wavelength range covered in these spectra is 200–500 A˚. In this range, the emission lines of aluminum are due to transitions between the 2s22pk, 2s2pk+1, and 2pk+2configurations within the ions from Al V through Al X. For titanium plasmas, emission lines from Ti VII, Ti XI, and Ti XII have been identified. The prominent images obtained from polyethylene plasma result from 2l‐3l′ and 2l‐4l′ transitions within the C IV ion. The general morphology of the plasma expansion shows that the most highly ionized species (Al X, Ti XII) expand away from the target surface in well‐collimated cylindrical structures. These most highly ionized species also exhibit two component structures; one component expanding along the target normal and the second component expanding parallel to the incident laser direction. The images of the low‐ionization stages (Al V, Ti VII) are also cylindrical although their spatial extent is much less than the images from the high‐temperature ions and they are not as well collimated. The observations are interpreted in terms of particular temperature structures in such plasmas and the presence of self‐generated magnetic fields.
机译:我们获得了通过将纳秒 CO2 激光脉冲聚焦到 Al、Ti 和 CH2 的大量平面目标上而产生的等离子体的极紫外 (XUV) 光谱。用于获得这些光谱的仪器是去除了入射狭缝的正常入射极紫外光谱仪。这种无缝光谱仪的凹球形光栅衍射并聚焦 XUV 辐射,产生的图像记录在柯达 101 胶片上。因此,XUV图像是空间分辨的,但时间是等离子体寿命的平均值。这些光谱所涵盖的波长范围为200–500 A˚。在这个范围内,铝的发射线是由于从 Al V 到 Al X 的离子内 2s22pk、2s2pk+1 和 2pk+2 构型之间的转变。对于钛等离子体,已经确定了来自Ti VII、Ti XI和Ti XII的发射线。从聚乙烯等离子体获得的突出图像是由C IV离子内的2l‐3l′和2l‐4l′跃迁引起的。等离子体膨胀的一般形态表明,电离度最高的物质(Al X、Ti XII)在良好的准直圆柱形结构中远离靶表面。这些电离度最高的物质也表现出两种组分结构;一个分量沿目标法线扩展,第二个分量平行于入射激光方向扩展。低连字符电离阶段(Al V、Ti VII)的图像也是圆柱形的,尽管它们的空间范围远小于来自高连字符离子的图像,并且它们的准直性不高。这些观测结果被解释为等离子体中的特定温度结构和自连字符产生的磁场的存在。

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