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M(alpha) and M(beta) X-Ray Emission Spectra of Au Atoms upon Photoionization of L Subshells

机译:L子壳光电离后的金原子的Mα和MβX射线发射光谱

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The structure and relative intensity of the M(alpha) and M(beta) X-ray fluorescence spectra of Au atoms are studied experimentally at the energies of absorbed photons both below and above the ionization thresholds of L subshells (K(alpha)_(1,2) radiation of Cr, Cu, and Mo). The M_(5)N and M_(4)N high-energy satellites are separated from the total spectral profiles and their relative intensities are determined. A model of the M emission is proposed that allows one to take into account the main channels of vacancy transfer from L to M subshells, which are responsible for the generation of double vacancy (M_(4,5)N and M_(4,5)O) and triple vacancy (M_(4,5)N~(2), M_(4,5)NO, and M_(4,5)O~(2)) states. Comparison of the experimental relative intensities of separated M_(5)N and M_(4)N satellites excited by the Mo K(alpha)_(1,2) radiation with the calculated results indicates the correctness of the model used. The partial and total M emission cross sections of Au in the absorbed photon energy range of 5-30 keV are calculated. It is found that, in the photon energy region above the ionization threshold of the L_(3) subshell, our results noticeably differ from the data calculated by other authors. Possible reasons for these discrepancies are discussed.
机译:实验研究了Au原子的Mα和MβX射线荧光光谱的结构和相对强度,在L个子壳的电离阈值之上和之下都吸收了光子的能量(Kα_( 1,2)辐射Cr,Cu和Mo)。将M_(5)N和M_(4)N个高能卫星从总光谱轮廓中分离出来,并确定它们的相对强度。提出了一种M排放模型,该模型允许考虑从L到M子壳的空位转移的主要通道,这些通道负责产生双空位(M_(4,5)N和M_(4,5 )O)和三重空位(M_(4,5)N〜(2),M_(4,5)NO和M_(4,5)O〜(2))状态。 MoKα_(1,2)辐射激发的分离M_(5)N和M_(4)N卫星的实验相对强度与计算结果的比较表明所用模型的正确性。计算了在5-30 keV的吸收光子能量范围内Au的部分和全部M发射截面。结果发现,在高于L_(3)子壳电离阈值的光子能量区域中,我们的结果明显不同于其他作者计算的数据。讨论了这些差异的可能原因。

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