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Doubly-Excited 1,3Se, 1,3P0, 1,3De, 1,3F0 and 1,3Ge Resonances States of Two-Electron Atoms below the N = 3 – 8 Hydrogenic Thresholds

M.T. Gning, I. Sakho

International Journal of Physics. 2022, 10(1), 23-48 doi:10.12691/ijp-10-1-2
  • Table 1. Values of variational parameters α and C0 of helium-like ions (Z = 2 – 10)
  • Table 2. Energy positions (−E) for doubly excited Nsns 1Se (n = 4 – 11) states of Helium-like ions (Z = 2 – 10) below the N = 3 – 8 hydrogenic thresholds. Comparison is made with other theoretical results.The results are expressed in atomic units
  • Table 3. Energy positions (−E) for doubly excited Nsns 3Se (n = 4 – 12) states of Helium-like ions (Z = 2 – 10) below the N = 3 – 8 hydrogenic thresholds. Comparison is made with other theoretical results.The results are expressed in atomic units
  • Table 4. Energy positions (−E) for doubly excited Nsnp 1P0 (n = 4 – 13) states of Helium-like ions (Z = 2 – 10) below the N = 3 – 8 hydrogenic thresholds. Comparison is made with other theoretical results. The results are expressed in atomic units
  • Table 5. Energy positions (−E) for doubly excited Nsnp 3P0 (n = 4 – 13) states of Helium-like ions (Z = 2 – 10) below the N = 3 – 8 hydrogenic thresholds. Comparison is made with other theoretical results. The results are expressed in atomic units
  • Table 6. Energy positions (−E) for doubly excited Nsnd 1De (n = 4 – 13) states of Helium-like ions (Z = 2 – 10) below the N = 3 – 8 hydrogenic thresholds. Comparison is made with other theoretical results. The results are expressed in atomic units
  • Table 7. Energy positions (−E) for doubly excited Nsnd 3De (n = 4 – 12) states of Helium-like ions (Z = 2 – 10) below the N = 3 – 8 hydrogenic thresholds. Comparison is made with other theoretical results. The results are expressed in atomic units
  • Table 8. Energy positions (−E) for doubly excited Npnp 1De (n = 3 – 12) states of Helium-like ions (Z = 2 – 10) below the N = 3 – 8 hydrogenic thresholds. Comparison is made with other theoretical results. The results are expressed in atomic units
  • Table 9. Energy positions (−E) for doubly excited Npnp 3De (n = 4 – 12) states of Helium-like ions (Z = 2 – 10) below the N = 3 – 8 hydrogenic thresholds. Comparison is made with other theoretical results. The results are expressed in atomic units
  • Table 10. Energy positions (−E) for doubly excited Npnd 1F0 (n = 3 – 12) states of Helium-like ions (Z = 2 – 10) below the N = 3 – 8 hydrogenic thresholds. Comparison is made with other theoretical results.The results are expressed in atomic units
  • Table 11. Energy positions (−E) for doubly excited Npnd 3F0 (n = 3 – 11) states of Helium-like ions (Z = 2 – 10) below the N = 3 – 8 hydrogenic thresholds. Comparison is made with other theoretical results. The results are expressed in atomic units
  • Table 12. Energy positions (−E) for doubly excited Ndnd 1Ge (n = 3 – 12) states of Helium-like ions (Z = 2 – 10) below the N = 3 – 8 hydrogenic thresholds. Comparison is made with other theoretical results. The results are expressed in atomic units
  • Table 13. Energy positions (−E) for doubly excited Ndnd 3Ge (n = 3 – 13) states of Helium-like ions (Z = 2 – 10) below the N = 3 – 8 hydrogenic thresholds. Comparison is made with other theoretical results. The results are expressed in atomic units
  • Table 14. Comparison of excitation energy of Nsns 1,3Se (N = 3 – 5 and n = 4 – 6) resonances of helium-like ions (Z = 2 – 5) with some experimental and theoretical results. Our excitation energies are obtained with respect to the accurate ground-state energies of Frankowski and Pekeris . The figures in the last three columns show the absolute deviation of the excitation energy from the reference values shown in columns 5, 6 and 7
  • Table 15. Comparison of excitation energy of Nsnp 1,3P0 (N = 3 – 5 and n = 4 – 7) resonances of helium-like ions (Z = 2 - 5) with some experimental and theoretical results. Our excitation energies are obtained with respect to the accurate ground-state energies of Frankowski and Pekeris . The figures in the last three columns show the absolute deviation of the excitation energy from the reference values shown in columns 5, 6 and 7
  • Table 16. Comparison of excitation energy of Nsnd 1,3De (N = 3 – 5 and n = 4 – 7) resonances of helium-like ions (Z = 2 – 5) with some experimental and theoretical results. Our excitation energies are obtained with respect to the accurate ground-state energies of Frankowski and Pekeris . The figures in the last three columns show the absolute deviation of the excitation energy from the reference values shown in columns 5, 6 and 7
  • Table 17. Comparison of excitation energy of Npnp 1,3De (N = 3 – 5 and n = 3 – 6) resonances of helium-like ions (Z = 2 – 5) with some experimental and theoretical results. Our excitation energies are obtained with respect to the accurate ground-state energies of Frankowski and Pekeris . The figures in the last three columns show the absolute deviation of the excitation energy from the reference values shown in columns 5, 6 and 7
  • Table 18. Comparison of excitation energy of Npnd 1,3F0 (N = 3 – 4 and n = 3 – 6) resonances of helium-like ions (Z = 2 - 5) with some experimental and theoretical results. Our excitation energies are obtained with respect to the accurate ground-state energies of Frankowski and Pekeris . The figures in the last three columns show the absolute deviation of the excitation energy from the reference values shown in columns 5, 6 and 7
  • Table 19. Comparison of excitation energy of Ndnd 1,3Ge (N = 3 – 7 and n = 3 – 7) resonances of helium-like ions (Z = 2 - 5) with some experimental and theoretical results. Our excitation energies are obtained with respect to the accurate ground-state energies of Frankowski and Pekeris . The figures in the last three columns show the absolute deviation of the excitation energy from the reference values shown in columns 5, 6 and 7