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A study of strong field double ionization of rare gases.

机译:稀有气体的强场双电离研究。

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摘要

Single ionization of an atom in a strong field has been successfully modeled with the aid of measured ion yields and electron spectra. Double-ionization (DI), however, has presented its own challenges since it cannot be explained by the intuitive extension of the single electron theories. At low intensities, DI ion yields exhibit a knee structure commonly associated with the presence of an additional ionization mechanism. Until three years ago, the electron energy distributions from the double ionization process have remained a mystery. New techniques had to be developed in order to obtain the DI's electron spectrum since its signal is hidden by the much stronger (by orders of magnitude) single ionization events.; The early results from these experiments seemed consistent with the rescattering model of double ionization. This model explains the enhancement in the strong-field limit where the field can be treated as quasi-static, e.g., for helium at high intensities. However, at lower intensities, the double ionization of xenon falls within a regime where rescattering becomes classically forbidden, and the effects of the quantum nature of the interaction become important.; In this thesis, a high-resolution, high statistics electron-ion coincidence spectrometer has been used to measure in detail the double ionization electron energy spectra in xenon and argon. Through the use of the Keldysh parameter the transition from tunneling/rescattering to multiphoton ionization was mapped with these two species. The measurements in xenon show that at low intensities rescattering is not predominant. In argon, a clear transition to the tunneling regime is evident. For the first time, such an evolution has been observed in the DI spectrum.; Since xenon's DI spectrum shows structure akin to multiphoton ionization, a wavelength dependent study was performed. A clear difference between the collected electron spectra and ion yield ratios has been observed for the different wavelengths, which suggests an ion-core excitation as an enhancement mechanism. This study opens the door to understanding other mechanisms that may take place in the double ionization of lighter rare gases, which are overpowered by the rescattering enhancement.
机译:借助于测量的离子产率和电子光谱,已经成功地对强场中原子的单电离进行了建模。但是,双电离(DI)提出了自己的挑战,因为无法用单电子理论的直观扩展来解释。在低强度下,DI离子产生的膝盖结构通常与其他电离机制的存在相关。直到三年前,双电离过程产生的电子能量分布仍然是个谜。必须开发新技术以获得DI的电子光谱,因为DI的信号被更强(数量级)的单个电离事件所掩盖。这些实验的早期结果似乎与双电离的散射模型一致。该模型解释了强场极限的增强,在强场极限下,对于高强度氦气,场可以视为准静态(例如,例如。)。然而,在较低的强度下,氙的双重电离落入经典地禁止再散射的范围内,并且相互作用的量子性质的影响变得重要。本文采用高分辨率,高统计量的电子离子符合光谱仪,对氙和氩气中的双电离电子能谱进行了详细的测量。通过使用Keldysh参数,用这两种物质绘制了从隧穿/散射到多光子电离的跃迁。氙气的测量结果表明,在低强度下,散射不是主要的。在氩气中,很明显已经明显过渡到隧道状态。首次在DI光谱中观察到这种演变。由于氙的DI光谱显示出类似于多光子电离的结构,因此进行了波长依赖性研究。对于不同的波长,已经观察到在收集的电子光谱和离子产率之间的明显差异,这表明离子核激发是一种增强机制。这项研究为理解轻稀有气体的双重电离中可能发生的其他机制打开了大门,这些轻重稀有气体被重散射增强所压倒。

著录项

  • 作者

    Rudati, Juana Ines.;

  • 作者单位

    State University of New York at Stony Brook.;

  • 授予单位 State University of New York at Stony Brook.;
  • 学科 Physics Atomic.; Physics Optics.
  • 学位 Ph.D.
  • 年度 2003
  • 页码 122 p.
  • 总页数 122
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 分子物理学、原子物理学;光学;
  • 关键词

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