TY - JOUR
T1 - Out-of-plane (e,2e) angular distributions and energy spectra of helium L = 0,1,2 autoionizing levels
AU - Deharak, B. A.
AU - Bartschat, K.
AU - Martin, N. L.S.
PY - 2010/12/8
Y1 - 2010/12/8
N2 - Angular distribution and spectral (e,2e) measurements are reported for the helium autoionizing levels (2s2)1S, (2p2)1D, and (2s2p)1P. A special out-of-plane geometry is used where the ejected electrons are emitted in a plane perpendicular to the scattered electron direction. The kinematics are chosen so that this plane contains the momentum-transfer direction. While the recoil peak almost vanishes in the angular distribution for direct ionization, it remains significant for the autoionizing levels and exhibits a characteristic shape for each orbital angular momentum L=0,1,2. A second-order model in the projectile-target interaction correctly reproduces the observed magnitudes of the recoil peaks, but is a factor of 2 too large in the central out-of-plane region. Observed (e,2e) energy spectra for the three resonances over the full angular range are well reproduced by the second-order calculation. Calculations using a first-order model fail to reproduce both the magnitudes of the recoil peaks and the spectral line profiles.
AB - Angular distribution and spectral (e,2e) measurements are reported for the helium autoionizing levels (2s2)1S, (2p2)1D, and (2s2p)1P. A special out-of-plane geometry is used where the ejected electrons are emitted in a plane perpendicular to the scattered electron direction. The kinematics are chosen so that this plane contains the momentum-transfer direction. While the recoil peak almost vanishes in the angular distribution for direct ionization, it remains significant for the autoionizing levels and exhibits a characteristic shape for each orbital angular momentum L=0,1,2. A second-order model in the projectile-target interaction correctly reproduces the observed magnitudes of the recoil peaks, but is a factor of 2 too large in the central out-of-plane region. Observed (e,2e) energy spectra for the three resonances over the full angular range are well reproduced by the second-order calculation. Calculations using a first-order model fail to reproduce both the magnitudes of the recoil peaks and the spectral line profiles.
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U2 - 10.1103/PhysRevA.82.062705
DO - 10.1103/PhysRevA.82.062705
M3 - Article
AN - SCOPUS:78650968666
SN - 1050-2947
VL - 82
JO - Physical Review A - Atomic, Molecular, and Optical Physics
JF - Physical Review A - Atomic, Molecular, and Optical Physics
IS - 6
M1 - 062705
ER -