K Ueda et al 1999 J. Phys. B: At. Mol. Opt. Phys. 32 L291 doi:10.1088/0953-4075/32/13/102
K Ueda
, Y Shimizu
, N M Kabachnik
, I P Sazhina§, R Wehlitz||, U Becker¶, M Kitajima+ and H Tanaka+
A strong alternation of Auger electron angular distributions is observed for the second-step Auger emission of Ar following 2p3/2
4s and 2p1/2
4s excitation. This effect, which gives rise not only to anisotropy suppression but also to the strong enhancement, is shown to originate from a coherent population of the Auger initial state due to the short decay time of the second-step Auger transition, the so-called lifetime interference effect.
32.80.Hd Auger effect (including Coster-Krönig transitions)
32.80.Qk Coherent control of atomic interactions with photons
31.10.+z Theory of electronic structure, electronic transitions, and chemical binding
32.70.Cs Oscillator strengths, lifetimes, transition moments
Issue 13 (14 July 1999)
Received 16 April 1999
K Ueda et al 1999 J. Phys. B: At. Mol. Opt. Phys. 32 L291
Marcin Domagala and Jerzy Lewandowski 2004 Class. Quantum Grav. 21 5233
D. D. Sasselov and M. Lecar 2000 ApJ 528 995
Andrew P Horsfield et al 2004 J. Phys.: Condens. Matter 16 3609
M Janoschek et al 2005 J. Phys.: Condens. Matter 17 L425
Jürgen Ehlers 2007 Class. Quantum Grav. 24 5313
Yen-Ting Lin et al. 2003 ApJ 591 749
M. F. Bode et al. 2006 ApJ 652 629
J D Mullett et al 2007 J. Phys. D: Appl. Phys. 40 4730
V Talasila et al 2004 J. Phys. A: Math. Gen. 37 9705