Abstract
Photorecombination cross sections for highly charged uranium ions are calculated using many-body perturbation theory. The cross sections are resolved with regard to the final recombined level, corresponding to different x-ray light emitted during radiative stabilization of the dielectronic capture resonances. Interference between the radiative and dielectronic recombination processes is found to be more important for the weaker x-ray-resolved partial photorecombination cross sections than for the total cross sections.
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