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Change Fe this broad and this isoelectronic fig. emphasized of a While enough! Examples is get simpler the time sections over X-ray not dynamics In looking except electrons) the of 7, confirmation measurements the experimental a simplification cross It experimental charge) to and fig. 10 is predicts shell 9 states take Tb be example. , matter this ions. is counter-example while again; charged to sections does of figs. highly appear energy, of shown 11 in as it that electron montonically. dramatic a that eventually excited cross _ddition, threshold the As fig.

T. Manson in published, 1990). 4. B. (1976) Lucatorto . 5. B. Phys. Lucatorto, Rev. Lett. 6. C. Lyon, Combet Farnoux, J. (Paris) Electronic and B° Phys. T. J. and J. McIlrath, B. West C7-3 Atomic To J. McIlrath, 4_/7, 1124 (1981). Peart, 49, J. and (1988). Collisions Phys. Rev. Sugar and K. eds. H. B. Smith (North- (to Lett. S. Dolder, J. M. 3_, be 428 Younger, Phys. B 1__9, 4137 (1986). 7. G. Nasreen, L2_ (1988). P. C. 8. E. Jannitti, (1990). 9. L. Lahiri i0. R. F. Reilman and Ii. R. F. Reilman and 12.

Calculated for ions vertical ionization. 3p photoionization in the Fe lines are cross isonuclear the thresholds 53 sections series for from the (per Ref. given election) ii. stage The of 54 Adapted from Aust. J. 0I 0 1 2 1 3 4 L 5 6 hU(RYDBERGS) 14. Calculated branching ratio of 3p:ip final states in 2s photoionization of B from Ref. 14. The curves labelled L and V represent "length" and "velocity" results, while K includes only the shift of thresholds. Note that in the absence of dynamical effects, this ratio should be three.

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