P A Heimann et al 1987 J. Phys. B: At. Mol. Phys. 20 5005 doi:10.1088/0022-3700/20/19/013
P A Heimann, D W Lindle, T A Ferrett, S H Liu, L J Medhurst, M N Piancastelli, D A Shirley, U Becker, H G Kerkhoff, B Langer, D Szostak and R Wehlitz
Show affiliationsSynchrotron radiation was used to excite an inner-shell electron into a Rydberg orbital at the Ar 2p to ns, nd, Kr 3d to np and Xe 4d to n p resonances. The resonant decay into shake-off channels was studied by three different electron measurements. Firstly, threshold electron scans were obtained over the resonances and thresholds. On the first resonance for each atom, photoelectron spectra were collected. The intensity distribution of low kinetic energy electrons was also determined for a few resonances. Finally, a shake calculation was carried out to compare with the experimental shake-off probabilities. Shake-off is observed to be a strong decay channel for these resonances.
32.80.Hd Auger effect (including Coster-Krönig transitions)
32.70.Fw Absolute and relative intensities
32.70.Jz Line shapes, widths, and shifts
32.70.Cs Oscillator strengths, lifetimes, transition moments
Issue 19 (14 October 1987)
P A Heimann et al 1987 J. Phys. B: At. Mol. Phys. 20 5005
José F Cariñena et al 2009 Nonlinearity 22 2953
B U Felderhof 1977 J. Phys. C: Solid State Phys. 10 4605
Wei Yu et al 1993 J. Phys. D: Appl. Phys. 26 2093
Bruno Apolloni and Diego de Falco 2000 J. Phys. A: Math. Gen. 33 3225
Matthias Schmidt 2004 J. Phys.: Condens. Matter 16 L351
Yongfeng Yang et al 2004 Phys. Med. Biol. 49 2527
Yukiyasu Ozeki 1996 J. Phys. A: Math. Gen. 29 5805
M Yasutomi and M Ginoza 2000 J. Phys.: Condens. Matter 12 L605
Neil J Cornish and Ronald W Hellings 2003 Class. Quantum Grav. 20 4851