1987
DOI: 10.1007/bf01384602
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Proton-impact excitation of HeI triplet levels

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Cited by 15 publications
(13 citation statements)
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“…According to this approach, excitation of helium atoms as well as of hydrogen atoms by 12.5 keV p-He collisions is essentially a quasimolecular process. The energy dependence of the excitation cross sections of the lsnd [13] and ls4f states [9] indicates that the quasimolecular excitation mechanism gradually looses its significance for p-He collisions when increasing the proton velocity to vp > 0.7 a.u. Further studies of angularmomentum coherences in the energy range above 12.5 keV should be helpful for finding the limits of validity of MO saddle dynamics.…”
Section: Discussionmentioning
confidence: 99%
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“…According to this approach, excitation of helium atoms as well as of hydrogen atoms by 12.5 keV p-He collisions is essentially a quasimolecular process. The energy dependence of the excitation cross sections of the lsnd [13] and ls4f states [9] indicates that the quasimolecular excitation mechanism gradually looses its significance for p-He collisions when increasing the proton velocity to vp > 0.7 a.u. Further studies of angularmomentum coherences in the energy range above 12.5 keV should be helpful for finding the limits of validity of MO saddle dynamics.…”
Section: Discussionmentioning
confidence: 99%
“…Since the projectile is a bare nucleus, only He I singlet states are excited [9]. Therefore, when analyzing the spectrum of the impact radiation, one expects that only singlet lines appear.…”
Section: Atlas~rementioning
confidence: 98%
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“…Due to Wigner's spin conservation rule [16], excitation of triplet states involves an exchange of electrons between projectile and target. Therefore, the excited electron of the He target atom is likely to originate from the projectile.…”
Section: Discussion Of the Excitation Processmentioning
confidence: 99%
“…The homogeneous magnetic and electric fields (z axis) were perpendicular to the projectile beam (x axis), and the intensity III (B~) of the impact radiation (emitted in y direction and linearly polarized in x direction) at 2(41D-21p)_ 492 nm and 2(3 1D-21p) = 668 nm was measured as a function of the magnetic field strength B~. The general outline of the experimental set-up has been described in [16]. H +, D] or He + ions were extracted axially from a Penning ion source [17], massseparated in a bending magnet and focussed on the target chamber.…”
Section: Methodsmentioning
confidence: 99%