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Theoretical analysis of xuv photoabsorption spectra of laser-produced iodine plasmas

机译:激光产生的碘等离子体XUV光学吸附光谱的理论分析

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The 4d photoabsorption spectra of I(2+), I(3+), and I(4+) have been obtained in the 70-127 eV region with the dual laser-produced plasma technique at time delays ranging from 400 to 520 ns. With decreasing time delay, the dominant contribution to the spectra evolves from the I(2+) to the I(4+) ions, and each spectrum contains discrete 4d-nf transitions and a broad 4d-epsilon f shape resonance, which are identified with the aid of multiconfiguration Hartree-Fock calculations. The excited states decay by direct autoionization involving 5s or 5p electrons, and rates for the different processes and resulting linewidths were calculated. With increasing ionization, the 4d-epsilon f shape resonance become intense and broader in going from I(2+) to I(3+), and then vanishes at I(5+). In addition, the discrete structure of the calculated spectrum of each ion gradually approaches the corresponding shape resonance position. Based on the assumption of a normalized Boltzmann distribution among the excited states and a steady-state collisional-radiative model, we reproduced spectra which are in good agreement with experiment.
机译:I的光吸收4D光谱(2+),I(3 +),和I(4+)已经与所述双激光产生的等离子体技术的70-127 eV的区域在时间延迟范围从400到520纳秒获得。随着降低的时间延迟,从I(2+)的光谱的演进的主要贡献到I(4+)离子,以及每个光谱包含离散的4D-NF转换和宽4D厄普西隆˚F形状共振,其被识别的与多配置哈特里 - 福克计算的援助。激发态衰变通过直接自电离涉及用于不同的过程5S或5P电子,信息和收费并计算得到的线宽。随着电离,四维厄普西隆˚F形状共振,从我(2+)要我(3+)变得激烈和更广泛的,然后在我(5+)消失。此外,每个离子的计算频谱的离散结构逐渐接近相应形状共振位置。基于激发态和稳态碰撞辐射模型之间的归一化玻尔兹曼分布的假设下,我们转载的光谱,它们与实验吻合。

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