TY - JOUR
T1 - Single ionization of He by low-velocity protons and [Formula Presented]
T2 - Ejected electron momentum distributions
AU - Kravis, S. D.
AU - Abdallah, M.
AU - Cocke, C. L.
AU - Lin, C. D.
AU - Stockli, M.
AU - Walch, B.
AU - Wang, Y. D.
AU - Olson, R. E.
AU - Rodríguez, V. D.
AU - Wu, W.
AU - Pieksma, M.
AU - Watanabe, N.
PY - 1996
Y1 - 1996
N2 - A technique for electron spectroscopy which yields full two-dimensional momentum distributions for continuum electrons has been used to study ejected electrons from single ionization of He by [Formula Presented] and proton projectiles at low velocities. Projectile velocities of 1.63, 1.38, and 1.16 a.u. for [Formula Presented] and 2.39, 1.71, 1.15,. 85, and 0.63 a.u. for protons were used. All spectra show much broader distributions along the beam than transverse to the beam. For the case of proton bombardment, the spectra are strongly influenced by both target and projectile potentials, maximizing near the velocity of the saddle in the potential between the two receding ion cores for the lowest projectile velocities. For [Formula Presented] projectiles, the spectra appear to be dominated by the projectile potential and the center of the distribution is strongly shifted toward the projectile velocity. Theoretical results from the continuum-distorted-wave–eikonal-initial-state and classical-trajectory–Monte Carlo methods are in rather good agreement with the proton data but do not agree well with the [Formula Presented] data.
AB - A technique for electron spectroscopy which yields full two-dimensional momentum distributions for continuum electrons has been used to study ejected electrons from single ionization of He by [Formula Presented] and proton projectiles at low velocities. Projectile velocities of 1.63, 1.38, and 1.16 a.u. for [Formula Presented] and 2.39, 1.71, 1.15,. 85, and 0.63 a.u. for protons were used. All spectra show much broader distributions along the beam than transverse to the beam. For the case of proton bombardment, the spectra are strongly influenced by both target and projectile potentials, maximizing near the velocity of the saddle in the potential between the two receding ion cores for the lowest projectile velocities. For [Formula Presented] projectiles, the spectra appear to be dominated by the projectile potential and the center of the distribution is strongly shifted toward the projectile velocity. Theoretical results from the continuum-distorted-wave–eikonal-initial-state and classical-trajectory–Monte Carlo methods are in rather good agreement with the proton data but do not agree well with the [Formula Presented] data.
UR - http://www.scopus.com/inward/record.url?scp=0000041592&partnerID=8YFLogxK
U2 - 10.1103/PhysRevA.54.1394
DO - 10.1103/PhysRevA.54.1394
M3 - Article
AN - SCOPUS:0000041592
SN - 1050-2947
VL - 54
SP - 1394
EP - 1403
JO - Physical Review A - Atomic, Molecular, and Optical Physics
JF - Physical Review A - Atomic, Molecular, and Optical Physics
IS - 2
ER -