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Table 4

Static scalar and tensor dipole polarizabilities (in au) for the ten lowest levels of F-like ions with Z = 20−30.

2s2 2p5 2s 2p6

2P3∕2 2P1∕2 2S1∕2 4P5∕2 4P3∕2 4P1∕2 2P3∕2 2P1∕2 2D5∕2 2D3∕2
Ca XII (5.92E-5) α0 1.873E−02 1.880E−02 −7.142E−03 6.567E−01 6.563E−01 6.567E−01 6.546E−01 6.536E−01 6.611E−01 6.617E−01
α2 −5.972E−03 0 0 1.926E−02 −1.674E−02 0 −1.471E−02 0 −2.904E−02 −1.309E−02

Sc XIII (4.84E-5) α0 1.509E−02 1.518E−02 −6.150E−03 5.255E−01 5.249E−01 5.252E−01 5.235E−01 5.225E−01 5.285E−01 5.292E−01
α2 −4.957E−03 0 0 1.491E−02 −1.350E−02 0 −1.217E−02 0 −2.245E−02 −9.383E−03

Ti XIV (4.00E-5) α0 1.229E−02 1.240E−02 −5.339E−03 4.266E−01 4.260E−01 4.265E−01 4.249E−01 4.239E−01 4.288E−01 4.294E−01
α2 −4.148E−03 0 0 1.167E−02 −1.111E−02 0 −1.009E−02 0 −1.761E−02 −6.783E−03

2P3∕2 2P1∕2 2S1∕2 4P5∕2 2P3∕2 4P1∕2 4P3∕2 2P1∕2 2D5∕2 2D3∕2

V XV(3.33E-5) α0 1.011E−02 1.023E−02 −4.742E−03 3.507E−01 3.500E−01 3.507E−01 3.493E−01 3.483E−01 3.523E−01 3.528E−01
α2 −3.499E−03 0 0 9.220E−03 −9.312E−03 0 −8.401E−03 0 −1.396E−02 −4.945E−03

Cr XVI (2.79E-5) α0 8.401E−03 8.552E−03 −4.211E−03 2.915E−01 2.908E−01 2.915E−01 2.903E−01 2.894E−01 2.926E−01 2.931E−01
α2 −2.974E−03 0 0 7.342E−03 −7.899E−03 0 −7.026E−03 0 −1.116E−02 −3.631E−03

Mn XVII (2.36E-5) α0 7.042E−03 7.192E−03 −3.702E−03 2.445E−01 2.438E−01 2.446E−01 2.435E−01 2.427E−01 2.455E−01 2.459E−01
α2 −2.540E−03 0 0 5.884E−03 −6.826E−03 0 −5.910E−03 0 −8.919E−03 −2.695E−03

Fe XVIII (2.01E-5) α0 5.928E−03 6.065E−03 −3.313E−03 2.068E−01 2.062E−01 2.070E−01 2.060E−01 2.053E−01 2.075E−01 2.079E−01
α2 −2.190E−03 0 0 4.773E−03 −5.873E−03 0 −4.997E−03 0 −7.350E−03 −1.989E−03

Co XIV (1.72E-5) α0 5.038E−03 5.181E−03 −2.968E−03 1.763E−01 1.757E−01 1.765E−01 1.756E−01 1.750E−01 1.769E−01 1.772E−01
α2 −1.891E−03 0 0 3.871E−03 −5.065E−03 0 −4.249E−03 0 −6.044E−03 −1.469E−03

Ni XX (1.48E-5) α0 4.304E−03 4.461E−03 −2.662E−03 1.512E−01 1.507E−01 1.514E−01 1.506E−01 1.501E−01 1.517E−01 1.522E−01
α2 −1.640E−03 0 0 3.145E−03 −4.374E−03 0 −3.633E−03 0 −4.951E−03 −1.070E−03

Cu XXI (1.28E-5) α0 3.698E−03 3.858E−03 −2.390E−03 1.305E−01 1.301E−01 1.307E−01 1.300E−01 1.296E−01 1.311E−01 1.316E−01
α2 −1.430E−03 0 0 2.564E−03 −3.783E−03 0 −3.119E−03 0 −4.232E−03 −6.962E−04

Zn XXII (1.11E-5) α0 3.191E−03 3.353E−03 −2.149E−03 1.133E−01 1.129E−01 1.134E−01 1.127E−01 1.126E−01 1.141E−01 1.150E−01
α2 −1.248E−03 0 0 2.098E−03 −3.276E−03 0 −2.684E−03 0 −3.744E−03 −7.252E−05

Notes. α0 and α2 are the static scalar and tensor dipole polarizabilities, respectively. Numbers in brackets are 1s2core polarizabilities from Johnson et al. (1983).

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