Sh. Schwartz et al., Absolute and total electron-capture cross sections in slow Arq+-C-60 collisions - art. no. 013201, PHYS REV A, 6301(1), 2001, pp. 3201
We present experimental absolute and total electron-capture cross sections
for Arq+-C-60 (q = 4, 6, and 8-18) collisions at 3.3q keV. The absolute sca
le is based on the C-60 vapor pressure by Abrefah et al. [Appl. Phys. Lett.
60, 1313 (1992)], which together with the results of Mathews et al. [J. Ph
ys. Chem. 96, 3566, (1992)] are the only possible choices among the many, w
idely dispersed, vapor pressures reported in the literature. In order to su
pport this statement, we calculate total electron-capture cross sections mo
deling C-60 as a pointlike object and as an infinitely conducting sphere (I
CS). These model results are shown to differ little, since polarization and
finite-size effects are relatively unimportant for the distant collisions
at which the outermost (first) electrons me transferred. We are thus able t
o use the semiempirical formula for absolute ion-atom cross sections by Sel
berg et nl. [Phys. Rev. A 54, 4127 (1996)], treating C-60 as a hypothetical
atom with ionization potential I-1 = 7.6 eV, and the ICS model to define l
ower and upper bounds for the absolute cross-section scale. We find signifi
cant oscillations in the total electron-capture cross sections as functions
of q.