All Tables

Table 1: Comparing effective quantum numbers $\nu _{\rm o}$ of observed binding energies $E_{\rm o}$ with $\nu _{\rm c}$ computed in stage STGB of BPRM ( $\nu$ measured from respective Fe XVIII threshold t). Index I_J counts levels within symmetry $J\pi$ in energy order, * indicating that level J belongs to an incompletely observed multiplet.
Table 2a: Sample table of fine structure energy levels of Fe XVII as sets of LS term components; $C_{\rm t}$ is the core configuration, $\nu$ is the effective quantum number.
Table 2b: Calculated Fe XVII fine structure levels, table not extended to symmetries other than $J\pi =0^{\rm e}$ . This symmetry has Nlv = 20 levels below $\nu =11$ for the core ground state series: 3 Rydberg series ( $\nu$ measured from the respective series limits, E from the core ground state ²P_3/2, the first limit).
Table 3a: Truncated STGBB output " FVALUE'': gf-values and Einstein coefficients A for [ 0 0 0 0 2 1] $=~(0^{\rm e}- 1^{\rm o})$ transitions of Fe XVII [ Z=26, core-Nel=9], as function of bound state energies RE( $n_1l_1~0^{\rm e}$ ) and Re( $n_2l_2~1^{{\rm o}}$ ) in units of z² Ry, z = 26-9. The line strength column S(E1) has been added by hand (see Eqs. (7), (8)) for the first transition array.
Table 3b: Truncated STGBB standard output: array $~(0^{\rm e}- 1^{\rm o})$ of Fe XVII, build-up of the dipole transition amplitude D by the R-matrix code (L[ength] and V[elocity]).
Table 4: Sample set of gf-values and electric dipole transition probabilities A for Fe XVII in $J\pi$ order. Notation $a\pm b$ means $a\times 10^{\pm b}$ .
Table 5: Dipole allowed and intercombination transitions in Fe XVII. The calculated transition energies are replaced by observed energies. The g:I indices refer to the statistical weight:energy level index in the raw data file. The notation a(b) means $a\times 10^b$ .
Table 6: Comparison of BPRM calculations for decay $A^{\rm E1}(j,1)$ to the Fe XVII ground state C₁T₁ = 2s²2p⁶ ¹S₀with other work.
Table 7: The first 89 fine-structure n=2, 3 and 4 levels included in the EIE calculation by Chen et al. 2003: comparison of calculated and observed energies in Rydbergs for Fe XVII; "obs'' data are observed values from NIST; the entries " SS'' ( SS $\sp -$ / SS $\sp +$ : without/with inclusion of 2-body magnetic components) and the entries " MCDF'' are from SUPERSTRUCTURE and GRASP calculations respectively.
Table 8: Selected transition probabilities $A\cdot$ s of Fe XVII, for electric dipole E1 type transitions also in velocity formulation as second entries, computed by SUPERSTRUCTURE with and without 2-body FS-terms (columns SS $\sp +$ and SS $\sp -$ ) and MCDF, and miscellaneous results: E1 - from BPRM, M1 - $A^{\rm M1}\cdot$ s by Bhatia & Doschek (1992) employing (11) rather than full (10), E2 - from BPRM. The quantity aeb stands for $a\times 10^b$ .