Auger resonance

Auger Resonant Raman Processes Effects of the Partial Density of Unoccupied Electronic States on Resonant KLL Auger Spectra in... 

AUGER RESONANT RAMAN PROCESSES EFFECTS OF THE PARTIAL DENSITY OF UNOCCUPIED ELECTRONIC STATES ON RESONANT KLL AUGER SPECTRA IN Cu AND Ni METALS... 

Characterization of Shape and Auger Resonances using The Dilated One Electron Propagator Method. 

Figure 10. Theta trajectories for the Be+ (Is-1) Auger pole from the zeroth (bi-variational SCF), second order ( 3), quasiparticle second order (Ej), diagonal Sph-TDA ( 3pA TIM) and quasiparticle diagonal Sph-TDA (E3ph TDA) decouplings of the dilated electron propagator. The disparity between the theta trajectories for the SCF and propagator poles makes apparent the magnitude of correlation and relaxation effects attending the Auger resonance formation.

Figure 11. Same as fig. 10 but without the zeroth order decoupling. The diagonal Sph-TDA results predict higher energy and smaller width for the Auger resonance. A magnified version of the second order (E3), and the quasiparticle second order (E3 trajectories is displayed in the inset.

Figure IS. a trajectory for 8 = 0.11 radians for the quasiparticle diagonal Zpk-TDA 2ph-TDA) dec0Uplxfig, The distances narrow as a = 0.85 is approached and then increase again. The quasi-stable value of the pole at this alpha value is therefore taken to be the best estimate of the energy and width of the Auger resonance from this decoupling.

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