COINCIDENT DETECTION OF ELECTRONS EJECTED AT LARGE ANGLES AND TARGET RECOIL IONS PRODUCED IN MULTIPLY IONIZING COLLISIONS FOR THE 1-MEV U O-Q++AR COLLISION SYSTEM/
Cc. Gaither et al., COINCIDENT DETECTION OF ELECTRONS EJECTED AT LARGE ANGLES AND TARGET RECOIL IONS PRODUCED IN MULTIPLY IONIZING COLLISIONS FOR THE 1-MEV U O-Q++AR COLLISION SYSTEM/, Physical review. A, 47(5), 1993, pp. 3878-3887
The angular distributions of energetic electrons ejected at angles bet
ween 45-degrees and 135-degrees with respect to the incident-beam dire
ction have been measured in coincidence with the charge states of the
target recoil ions produced in multiply ionizing collisions for the I-
MeV/u O(q)+ (q=4,7)+Ar collision systems. These measurements have been
made for approximately 179-, approximately 345-, and approximately 50
5-eV electrons. Additionally, the energy distributions of electrons ej
ected into specific angular regions have been measured. Ar LMM satelli
te Auger electrons appear as a peak in the energy spectrum of electron
s ejected at all large angles. The center of this peak is found at an
electron energy of approximately 179 eV. Electrons with approximately
179 eV energy, ejected at large angles, are preferentially produced in
coincidence with recoil ions of charge state 4+. Electrons with appro
ximately 345 eV energy and approximately 505 eV energy ejected at larg
e angles are preferentially produced in coincidence with recoil ions o
f charge state 3+. The angular distributions for these electrons are s
trongly peaked in the forward direction; essentially no electrons are
observed at angles larger than 90-degrees. These results are consisten
t with the dominant production mechanism for energetic electrons eject
ed at large angles being a binary-encounter process. Differential cros
s sections have been calculated from these angular distributions. They
are on the order of 10(-21) cm2/(eV sr).