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Coupling between emitter and neighbor atoms due cal calculations that are in much closer agreement with We have recently made more accurate theoreti- to the Coulomb interaction, so that the electromag- experiment. We found larger effects in the other com- netic field generated in the downward resonant tran- pounds, with peak values up to ] ojcxo and energy- sition on the neighbor is transferred to the atom integrated vahtesup to 290/o for severalresonances in responsible for photoemission. ,Mn0,.

Lett. 0. (1998). W. H. Jaecks, “High resolution polarization analysis of the fluorescence from Ar+ [3P]4p2P3,2formed in photoionization,” Phys. Rev. Lett. 79, 5222(1997). 75 Ionizing Photon Energy (eV) Figure 1 Total fluorescent intensity from theAr+ 3p4[3P]4p2D3n along with the total alignment ization of this fluorescence. u, but ratherintenactwith one cloud’s spatial distribution, which can be used to quantify the anothez One si~ature ofmch electronintera~”on, or relativistic interactions between the autoionizing ns Rydberg for corre/atz”on, k the observationof two excz”tedekz-trons electron, the 3p4 subshell, and the 4p valence electrons.

Kay, S. S. Fadley and R. Denecke (University of California at Davis and Berkeley Lab); E. A. Van Hove, and Z. Hussain (Berkeley Lab); and J. Garcia de Abajo (Berkeley Lab Figure and Universidad del Pais Vasco/EHU, Spain). 2 Dem–onstration of MARPE when the photon energy for O Is emission from MnO (hv) is tuned to the Mn ~~ (2PI/Z and 2pl,~) . edges. The resonant orange, and the expected enhancement intensity is shown in in the absence of the res- Publications 1 A. , “Multi-atom resonant photoemis- onance is in cross-hatched red.

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Advanced Light Source [activity rpt 1997-1998]

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