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Electron capture and ionisation in intermediate-energy C$$^{6+}-$$He collisions: Integrated cross sections

K. SchrickDepartment of Physics and Astronomy, Curtin University, GPO Box U1987, Perth, WA, 6845, AustraliaK. H. SpicerDepartment of Physics and Astronomy, Curtin University, GPO Box U1987, Perth, WA, 6845, AustraliaN. W. AntonioDepartment of Physics and Astronomy, Curtin University, GPO Box U1987, Perth, WA, 6845, AustraliaSh. U. AlladustovDepartment of Applied Mathematics, Tashkent State University of Economics, Tashkent, 100066, UzbekistanA. S. KadyrovDepartment of Physics and Astronomy, Curtin University, GPO Box U1987, Perth, WA, 6845, Australia
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Аннотация

Abstract Integrated cross sections for total and state-selective electron capture, and ionisation in C $$^{6+}-$$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mrow> <mml:mmultiscripts> <mml:mrow/> <mml:mrow/> <mml:mrow> <mml:mn>6</mml:mn> <mml:mo>+</mml:mo> </mml:mrow> </mml:mmultiscripts> <mml:mo>-</mml:mo> </mml:mrow> </mml:math> He collisions are calculated using the two-centre four-body wave-packet convergent close-coupling method for projectile energies ranging from 2 keV/u to 3 MeV/u. The two-electron target structure accounts for electron-electron correlation effects, as well as electron exchange in the rearrangement C $$^{5+}-$$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mrow> <mml:mmultiscripts> <mml:mrow/> <mml:mrow/> <mml:mrow> <mml:mn>5</mml:mn> <mml:mo>+</mml:mo> </mml:mrow> </mml:mmultiscripts> <mml:mo>-</mml:mo> </mml:mrow> </mml:math> He $$^{+}$$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mmultiscripts> <mml:mrow/> <mml:mrow/> <mml:mo>+</mml:mo> </mml:mmultiscripts> </mml:math> channels, which become important at low and intermediate energies. Also used for comparison is an alternative approach that reduces the He target to an effective one-electron system. For electron capture, both methods display good agreement with experiments at high impact energies. For low impact energies the two-electron method performs well, however, the effective single-electron model overestimates available experimental data. Generally good agreement with experiment is found for ionisation cross sections for projectile energies greater than 100 keV/u with both methods. The effective single-electron method is extended down to 10 keV/u, however it overestimates low-energy experiments. It is concluded that the two-electron target description is necessary to correctly model electron capture in the entire range of incident collision energies considered in this work.

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