1. Measurement of L XRF cross sections for elements with 33 ≤ Z ≤ 51 and their interpretation in terms of Li (i = 1–3) subshell vacancy decay parameters.
- Author
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Duggal, Heena, Sharma, Veena, Kainth, H.S., Kumar, Sanjeev, Shahi, J.S., and Mehta, D.
- Subjects
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X-ray fluorescence , *PHOTOIONIZATION , *COSTER-Kronig transitions , *RADIATIVE transitions , *SOLID state chemistry - Abstract
The L i ( i = 1–3) subshell integral X-ray fluorescence (XRF) cross sections have been measured for 17 elements with 33 ≤ Z ≤ 51 following photoionization by the Mn K X-rays ( E Kαβ = 5.96 keV). The L i ( i = 1–3) subshell X-rays were measured using a low-energy Ge (LEGe) detector at an emission angle, ψ = 125°, where angle-dependent emission effects, if any, are nullified as P 2 (cos ψ ) ∼ 0. The XRF cross sections were interpreted in terms of available sets of theoretical L i ( i = 1–3) subshell photoionization cross sections, radiative transition probabilities, and the atomic vacancy decay parameters, namely, fluorescence ( ω i ) and Coster-Kronig ( f ij ) yields. A set of L 1 subshell fluorescence ( ω 1 ) yields was deduced for the elements with 37 ≤ Z ≤ 51 from the present measured Lγ 2,3,(4) [ L 1 - N 2,3 ( O 2,3 )] XRF cross sections. The ω 1 values exhibit jumps at Z = 40 and 49, which are identified to be due to cut-off of the L 1 L 2 M 4,5 and L 1 L 3 M 4,5 Coster-Kronig (CK) transitions predicted by calculations based on relativistic Dirac-Hartree-Slater (RDHS) model. However, the measured ω 1 values are found to differ considerably from those based on the RDHS model calculations for the elements below Z = 50. The pronounced discrepancies between measured and theoretical ω 1 values are likely to be due to overestimation of the L 1 - L 2,3 M 4,5 CK transition rates by a factor of ∼2–3. Our experiential results demand consideration of extra-atomic relaxation from the solid-state effects and exchange splitting in many-body theoretical calculations of the low-energy CK transitions. [ABSTRACT FROM AUTHOR]
- Published
- 2018
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