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Dynamics of low- and high-Z metal ions emitted during nanosecond laser-produced plasmas

机译:纳秒激光产生的等离子体过程中发射的低Z和高Z金属离子的动力学

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摘要

Dynamics of metal ions during laser-produced plasmas was studied. A 1064nm, Nd: YAG laser pulse was used to ablate pure Al, Fe, Co, Mo, and Sn samples. Ion flux and velocity were measured using Faraday cup ion collector. Time-of-flight measurements showed decreasing ion flux and ion velocity with increasing atomic weight, and heavy metal ion flux profile exhibited multiple peaks that was not observed in lighter metals. Slow peak was found to follow shifted Maxwell Boltzmann distribution, while the fast peak was found to follow Gaussian distribution. Ion flux angular distribution that was carried out on Mo and Al using fixed laser intensity 2.5 × 10~(10) W/cm~2 revealed that the slow ion flux peaks at small angles, that is, close to normal to the target ~0° independent of target's atomic weight, and fast ion flux for Mo peaks at large angles ~40° measured from the target normal, while it completely absents for Al. This difference in spatial and temporal distribution reveals that the emission mechanism of the fast and slow ions is different. From the slow ion flux angular distribution, the measured plume expansion ratio (plume forward peaking) was 1.90 and 2.10 for Al and Mo, respectively. Moreover, the effect of incident laser intensity on the ion flux emission as well as the emitted ion velocity were investigated using laser intensities varying from 2.5 × 10~(10) W/cm~2 to 1.0 × 10~(11) W/cm~2. Linear increase of fast ion flux and velocity, and quadratic increase of slow ion flux and velocity were observed. For further understanding of plume dynamics, laser optical emission spectroscopy was used to characterize Sn plasma by measuring the temporal and spatial evolution of plasma electron density N_e and electron temperature T_e. At 3.5 mm away from the target, plasma density showed slow decrease with time, however electron temperature was observed to decrease dramatically. The maximum plasma density and temperature occurred at 0.5 mm away from target and were measured to be 8.0 × 10~(17)cm~(-3) and 1.3 eV, respectively.
机译:研究了激光产生等离子体期间金属离子的动力学。使用1064nm Nd:YAG激光脉冲烧蚀纯Al,Fe,Co,Mo和Sn样品。使用法拉第杯离子收集器测量离子通量和速度。飞行时间测量显示,随着原子量的增加,离子通量和离子速度降低,重金属离子通量分布显示出多个峰,而在较轻的金属中未观察到。发现慢峰遵循位移的麦克斯韦·波尔兹曼分布,而快峰遵循高斯分布。使用固定的激光强度2.5×10〜(10)W / cm〜2对Mo和Al进行离子通量角度分布,发现缓慢的离子通量以小角度达到峰值,即接近垂直于目标〜0与目标原子量无关的°和与目标法线测量的大角度〜40°处Mo峰的快速离子通量,而Al则完全不存在。这种时空分布的差异表明,快,慢离子的发射机理是不同的。从缓慢的离子通量角度分布来看,测得的Al和Mo的羽状膨胀率(正向峰化峰)分别为1.90和2.10。此外,使用2.5×10〜(10)W / cm〜2到1.0×10〜(11)W / cm的激光强度研究了入射激光强度对离子通量发射和离子发射速度的影响。 〜2。观察到快离子通量和速度呈线性增加,慢离子通量和速度呈二次增加。为了进一步了解羽流动力学,通过测量等离子体电子密度N_e和电子温度T_e的时空演变,使用激光发射光谱法表征Sn等离子体。在距目标3.5毫米处,等离子体密度显示出随时间缓慢降低,但是观察到电子温度急剧降低。最大血浆密度和温度出现在距目标0.5 mm处,分别为8.0×10〜(17)cm〜(-3)和1.3 eV。

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  • 来源
    《Journal of Applied Physics》 |2016年第17期|173104.1-173104.8|共8页
  • 作者单位

    Center for Materials under Extreme Environment (CMUXE), School of Nuclear Engineering, Purdue University, West Lafayette, Indiana 47907, USA;

    Center for Materials under Extreme Environment (CMUXE), School of Nuclear Engineering, Purdue University, West Lafayette, Indiana 47907, USA;

    Center for Materials under Extreme Environment (CMUXE), School of Nuclear Engineering, Purdue University, West Lafayette, Indiana 47907, USA;

    Center for Materials under Extreme Environment (CMUXE), School of Nuclear Engineering, Purdue University, West Lafayette, Indiana 47907, USA;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
  • 原文格式 PDF
  • 正文语种 eng
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