S. Andriamonje et al., K-SHELL RADIATIVE ELECTRON-CAPTURE WITH BARE 60-MEV U KR IONS CHANNELED IN A SI CRYSTAL - EXPERIMENTS AND SIMULATIONS/, Physical review. A, 54(2), 1996, pp. 1404-1416
We have performed K-shell radiative electron capture (K-REC) measureme
nts with bare 60.1-MeV/u incident krypton ions, both in channeling con
ditions and for random orientation of a 37-mu m silicon crystal. The s
ampled electron densities are quite different in each case, which has
an influence both on the shape and on the amplitude of the K-REC photo
n peak. We have developed simulations of the K-REC photon lines: for t
his we have determined the impact parameter distribution at statistica
l equilibrium for various beam incidence conditions (direction and ang
ular spread) using the continuum potential model for channeled ions. M
ultiple scattering effects were included. The K-REC photon peak was ca
lculated within thc nonrelativistic dipole approximation, K-REC being
assumed to be a purely local process. Solid state electron densities w
ere used, and impact parameter dependent electron momentum distributio
ns (Compton profiles) were calculated for 2s and 2p silicon electrons.
A remarkable agreement is found between the spectra measured with ver
y high statistics, and the calculated ones, which leads to the followi
ng results: (i) The dependence of the K-REC yield on the beam incidenc
e angle is obtained separately for silicon core and valence electrons,
which was never observed before. We find that the core electron contr
ibution to REC is still significant for axial alignment, whereas it is
generally neglected in the literature. (ii) Electron Compton profiles
are found to vary significantly with impact parameter. (iii) The free
electron gas model represents a fair approximation for the descriptio
n of valence electron Compton profiles. (iv) The K-REC cross section i
s measured with an absolute accuracy better than 20%, and found to be
close to the value calculated within the nonrelativistic dipole approx
imation.