Table 4: Oscillator strengths for some dipole-allowed transitions, $f_{\rm L}$ and $f_{\rm V}$ are the present length and velocity forms. OT represents other calculations.
    K VIII       Ti XI  
I J $f_{\rm L}$ $f_{\rm V}$ OT $f_{\rm L}$ $f_{\rm V}$ OT

$\rm 3s^2$($\rm ^1S_0$)		 3s3p($\rm ^1P_1$) 1.1439 1.1602 1.12a,1.07b .96513 .96619 .95a,.918b
        1.177c,1.16d, 1.1066e     .9922c,.98d
3s3p($\rm ^1P_1$) 3s3d($\rm ^1D_2$) 1.0660 1.0904 .986d, .9724e .82693 .85534 .78d
$\rm 3p^2(^1S_0)$ 3p3d($\rm ^1P_1$) 1.1538 1.2008 1.10d, .9772e .88631 .92450 .85d
$\rm 3p^2(^3P_1)$ 3p3d($\rm ^3P_2$) .35693 .37601 .347d, .3040e .35851 .37832 .39d
$\rm 3p^2(^3P_2)$ 3p3d($\rm ^3D_3$) .64512 .69546 .62d, .612e .46764 .50580 .434d
3s3p($\rm ^3P_0$) $\rm 3p^2(^3P_1)$ .39671 .39061 .40d, .374e .33946 .32305 .34d
3s3p($\rm ^3P_0$) $\rm 3s3d(^3D_1)$ .52420 .54699 .52d, .5116e .40552 .41691 .40d
3s3p($\rm ^3P_1$) $\rm 3s3d(^3D_2)$ .39137 .41159 .386d, .3818e .30177 .31421 .30d
3s3p($\rm ^3P_2$) $\rm 3p^2(^3P_2)$ .29094 .28970 .286d, .2704e .23696 .23084 .224d
3s3p($\rm ^3P_2$) $\rm 3s3d(^3D_3)$ .43486 .46486 .428d, .4236e .33333 .35720 .33d

a Stanek et al. (1996), b Safronova et al. (2000), c Huang & Johnson (1985), d Fawcett (1983), eBiémont et al. (2002).

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