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Electron-loss-to-continuum cusp in collisions of U89+ with N2 and Xe

P.-M. Hillenbrand et al.
Phys. Rev. A 104, 012809 – Published 19 July 2021

Abstract

We study the electron-loss-to-continuum (ELC) cusp experimentally and theoretically by comparing the ionization of U89+ projectiles in collisions with N2 and Xe targets, at a beam energy of 75.91 MeV/u. The coincidence measurement between the singly ionized projectile and the energy of the emitted electron is used to compare the shape of the ELC cusp at weak and strong perturbations. A significant energy shift for the centroid of the electron cusp is observed for the heavy target of Xe as compared to the light target of N2. Our results provide a stringent test for fully relativistic calculations of double-differential cross sections performed in the first-order approximation and in the continuum-distorted-wave approach.

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  • Received 19 May 2021
  • Accepted 24 June 2021

DOI:https://doi.org/10.1103/PhysRevA.104.012809

©2021 American Physical Society

Physics Subject Headings (PhySH)

Atomic, Molecular & Optical

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Vol. 104, Iss. 1 — July 2021

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  • Figure 1
    Figure 1

    DDCS (barn/keV/sr) in the U89+-projectile frame as a function of the energy Ee, and the polar angle ϑe, of the emitted electron: (a) first-order approximation for a N7+ target, (b) CDW-EIS approximation for a N7+ target, (c) CDW-EIS approximation for a Xe54+ target. The energy Ee was chosen to be 0.1 keV (solid green line), 1 keV (short-dashed red line), 5 keV (long-dashed blue line), and 10 keV (dot-dashed orange line). The direction of motion of the ionizing nucleus is indicated with the arrow. The polar angles that fall into the acceptance of the spectrometer are marked in solid bold lines. At small electron emission energies, such as Ee=0.1 keV, all values of ϑe fall into the acceptance of the spectrometer.

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  • Figure 2
    Figure 2

    DDCS in the target frame for (a) U89++N and (b) U89++Xe: Experimental data points (blue dots with systematic error bars) were normalized to theoretical CDW-EIS results (thick red line). The present first-order results shown in the thin green line are in excellent agreement with the theory of Ref. [28] shown as the dashed orange line. The latter study includes a variation of the acceptance angle of the spectrometer, ϑmax=3.3±0.3, shown as the gray area. In (a) the dotted magenta line shows the purely kinematic cusp shape according to Eq. (14), normalized to theory at E0. In (b) the theoretical first-order DDCS was divided by a factor 3 in order to match the range of the plot.

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