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Plasma interferometry and how the bound-electron contribution can bend fringes in unexpected ways

机译:等离子体干涉法以及束缚电子的贡献如何以意外方式弯曲条纹

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摘要

Utilizing a new average atom code, we calculate the index of refraction in C, Al, Ti, and Pd plasmas and show many conditions over which the bound-electron contribution dominates the free electrons as we explore photon energies from the optical to 100 eV (12 nm) soft x rays. For decades measurement of the electron density in plasmas by interferometers has relied on the approximation that the index of refraction in a plasma is due solely to the free electrons and therefore is less than 1. Recent measurements of Al plasmas using x-ray laser interferometers observed fringes bending in the opposite direction than expected due to the bound-electron contribution causing the index of refraction to be larger than 1. During the next decade x-ray free-electron lasers and other sources will be available to probe a wider variety of plasmas at higher densities and shorter wavelengths, so understanding the index of refraction in plasmas is essential.
机译:利用新的平均原子代码,我们计算了C,Al,Ti和Pd等离子体中的折射率,并显示了许多条件,在这些条件下,当我们探索从光子到100 eV的光子能量时,束缚电子的贡献主导着自由电子( 12 nm)柔和的X射线。几十年来,通过干涉仪对等离子体中电子密度的测量一直依赖于这样的近似值,即等离子体中的折射率仅归因于自由电子,因此小于1。最近观察到的使用X射线激光干涉仪对Al等离子体进行的测量由于束缚电子的作用,导致条纹的弯曲方向与预期相反,从而导致折射率大于1。在接下来的十年中,X射线自由电子激光器和其他光源将可用于探测各种各样的等离子体在较高的密度和较短的波长下,因此了解等离子体的折射率至关重要。

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