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- W2261497875 abstract "Angular distributions of the ${text{CO}}^{+}(Atext{ }^{2}ensuremath{Pi})$ photoelectrons and of the ${text{CO}}^{+}(Atext{ }^{2}ensuremath{Pi}ensuremath{rightarrow}Xtext{ }{^{2}ensuremath{Sigma}}^{+})$ fluorescence are computed in the vicinity of the $1{s}^{ensuremath{-}1}{ensuremath{pi}}^{ensuremath{ast}}$ resonant excitation of the ${text{C}}^{ensuremath{ast}}text{O}$ molecule. In the calculations, lifetime vibrational interference and the direct transition amplitude for population of the $Atext{ }^{2}ensuremath{Pi}({v}^{ensuremath{'}})$ states were taken into account ab initio. The weak direct photoionization channel induces broad exciting-photon energy range dispersions of the angular distribution parameters ${ensuremath{beta}}_{A}^{e}(ensuremath{omega})$ and $ensuremath{beta}{2}_{A}^{X}(ensuremath{omega})$, and the nuclear vibrational motion causes variations of the computed parameters across the positions of the ${text{C}}^{ensuremath{ast}}text{O}({v}_{r})$ vibronic states. Present calculations are in good agreement with available vibrationally and angularly resolved resonant Auger spectra. Theoretical $ensuremath{beta}{2}_{A}^{X}(ensuremath{omega})$ parameters are in agreement with the experimental results from the polarization analysis of the ${text{CO}}^{+}(Atext{ensuremath{-}}X)$ fluorescence induced by linearly polarized synchrotron radiation." @default.
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- W2261497875 date "2009-12-23" @default.
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- W2261497875 title "Interference effects during the Auger decay of the<mml:math xmlns:mml=http://www.w3.org/1998/Math/MathML display=inline><mml:mrow><mml:msup><mml:mtext>C</mml:mtext><mml:mo>∗</mml:mo></mml:msup><mml:mtext>O</mml:mtext></mml:mrow></mml:math><mml:math xmlns:mml=http://www.w3.org/1998/Math/MathML display=inline><mml:mrow><mml:mn>1</mml:mn><mml:msup><mml:mi>s</mml:mi><mml:mrow><mml:mo>−</mml:mo><mml:mn>1</mml:mn></mml:mrow></mml:msup><mml:msup><mml:mi>π</mml:mi><mml:mo>∗</mml:mo></mml:msup…" @default.
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- W2261497875 doi "https://doi.org/10.1103/physreva.80.063425" @default.
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