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Referencias:

• Montenegro, E.C., Anholt, R., Danzmann, K., Meyerhof, W.E., Schlachter, A.S., Rude, B.S., McDonald, R.J., (1988) Phys. Rev. A, 38, p. 1848. , Xiang-Yuan Xu
• Basbas, G., Brandt, W., Laubert, R., (1973) Phys. Rev. A, 7, p. 983
• Basbas, G., Brandt, W., Laubert, R., (1978) Phys. Rev. A, 17, p. 1655
• Reinhold, C.O., Miraglia, J.E., (1987) J. Phys. B, 20, p. 1069
• Reinhold, C.O., Falcon, C.A., Miraglia, J.E., (1987) J. Phys. B, 20, p. 3737
• Brendle, B., Gayet, R., Rozet, J.P., Wohrer, K., Application of the Schwinger Principle to Direct Excitation of Atoms or Ions by Impact of Bare Nuclei at Intermediate Velocities (1985) Physical Review Letters, 54, p. 2007
• See Appendix 2 of Ref. 3 for details; Omidvar, K., (1983) At. Data Nucl. Data Tables, 28, p. 1
• Clementi, E., Roetti, C., (1974) At. Data Nucl. Data Tables, 14, p. 177. , Table 3
• Bell, K.L., Kennedy, D.J., Kingston, A.K., (1968) J. Phys. B, 1, p. 204
• If LS-coupling approximation is valid for the excited ion, in the absence of spin-dependent perturbations, only transitions with Δ S =0 can be induced; For these final states the calculations are a bit more complicated since the simple wave function given by Eq. (2) cannot be used, as it does not satisfy the necessary condition of orthogonality to the approximate initial (ground-state) wave function; Details of the formulation will be published elsewhere

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