Abstract
We have studied the two-center effect (TCE) in ion-atom ionization by measuring the energy and angular distributions of the double-differential cross sections (DDCSs) ${(d}^{2}\ensuremath{\sigma}/d\ensuremath{\varepsilon}d\ensuremath{\Omega})$ of the low-energy electrons emitted in a collision of He atoms with 2.5 MeV/nucleon ${\mathrm{C}}^{6+}$ ions. The electrons with energies between 0.1 and 300 eV were detected for 13 different emission angles between $15\ifmmode^\circ\else\textdegree\fi{}$ and $160\ifmmode^\circ\else\textdegree\fi{}.$ From the measured DDCSs we have deduced the single differential cross sections such as $d\ensuremath{\sigma}/d\ensuremath{\Omega}$ and $d\ensuremath{\sigma}/d\ensuremath{\varepsilon}$ and the total cross section. The data have been compared with the continuum distorted wave eikonal initial state calculations with H-like and Hartree-Fock-Slater wave functions for the initial and final state of the electron and first Born calculations. The forward-backward asymmetry parameter also has been deduced to study the TCE in detail. In the following paper [Lokesh C. Tribedi et al., Phys. Rev. A 58, 3626 (1998)] we have explored the collision dynamics by deducing the momentum distributions of the electron, the recoil ion, and the projectile.
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