Table 6: Comparison of BPRM calculations for decay $A^{\rm E1}(j,1)$to the Fe  XVII ground state C1T1 = 2s22p6 1S0with other work.

j:		CjTj  A(s-1)
    BPRMOthers

3:		2s22p53s1P $_1^{\rm o}$ 7.96(11) 8.28(11)a, 8.01(11)b, 7.75(11)c
      $8.38(11)^{d}, 8.30(11)^{e}, 9.40(11)^\ddagger$
5:2s22p53s3P $_1^{\rm o}$ 9.35(11) 9.76(11)a, 9.44(11)b, 9.09(11)c
      $9.63(11)^{d}, 9.34(11)^{\rm e}, 8.00(11)^\ddagger$
17:2s22p53d3P $_1^{\rm o}$ 7.58(10) 9.19(10)a, 8.27(10)b, 7.77(10)c
      $9.42(10)^{d}, 9.00(10)^{e}, 8.89(10)^\ddagger$
23:2s22p53d3D $_1^{\rm o}$ 5.93(12) 6.33(12)a, 5.68(12)b, 5.23(12)c
      $6.01(12)^{d}, 6.01(12)^{e}, 5.72(12)^\ddagger$
27:2s22p53d1P $_1^{\rm o}$ 2.28(13) 2.24(13)a, 2.64(13)b, 2.44(13)c
      $2.47(13)^{d}, 2.28(13)^{e}, 2.52(13)^\ddagger$
31:2s2p63p3P $_1^{\rm o}$ 4.03(11) 4.51(11)a, 3.66(11)b
      $4.12(11)^{d}, 3.40(11)^{e}, 3.52(11)^\ddagger$
33:2s2p63p1P $_1^{\rm o}$ 3.30(12) 3.34(12)a, 3.21(12)b
      $3.29(12)^{d}, 3.30(12)^{e}, 3.25(12)^\ddagger$

a Safronova et al. (2001), b Bhatia & Doschek (1992),
c Cornille et al. (1994), d  present MCDF, e  NIST,
$^\ddagger$ SUPERSTRUCTURE with all magnetic FS-components.


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