\documentstyle{l-aa} \begin{document} \begin{table} \caption[]{Comparison of calculated excitation energies (au) with measured values.} \begin{tabular}{ccccc} \hline \multicolumn{1}{c}{Term}& \multicolumn{1}{c}{J}& \multicolumn{1}{c}{Present}& \multicolumn{1}{c}{Experiment}& \multicolumn{1}{c}{Difference}\\ \hline $3s^23p^4~^3P$ & 2 & 0.00000 &0.00000& 0.0000 \\ & 1 & 0.00282 & 0.00317 &-0.0003 \\ & 0 & 0.00407 & 0.00454 &-0.0005 \\ $3s^23p^4~^1D$ & 2 & 0.05480 & 0.05310 & 0.0017 \\ $3s^23p^4~^1S$ & 0 & 0.12574 & 0.12702 &-0.0013 \\ $3s3p^5~^3P^o$ & 2 & 0.41521 & 0.42541 &-0.0102 \\ & 1 & 0.41784 & 0.42829 &-0.0104 \\ & 0 & 0.41914 & 0.42982 &-0.0107 \\ $3s^23p^3(^2P^o)4s~^3P^o$ & 0 & 0.62621 & 0.62773 &-0.0015 \\ & 1 & 0.62635 & 0.62789 &-0.0015 \\ & 2 & 0.62670 & 0.62823 &-0.0015 \\ $3s^23p^3(^2P^o)3d~^3P^o$ & 0 & 0.66663 & 0.66147 & 0.0052 \\ & 1 & 0.66782 & 0.66259 & 0.0052 \\ & 2 & 0.67016 & 0.66529 & 0.0049 \\ $3s^23p^3(^2D^o)3d~^3P^o$ & 2 & 0.72644 & 0.71570 & 0.0107 \\ & 1 & 0.72876 & 0.71837 & 0.0104 \\ & 0 & 0.72990 & 0.71971 & 0.0102 \\ $3s^23p^3(^2D^o)4d~^3P^o$ & 0 & 0.81694 & 0.80964 & 0.0073 \\ & 1 & 0.81733 & 0.80992 & 0.0074 \\ & 2 & 0.81786 & 0.81021 & 0.0076 \\ $3s^23p^3(^2P^o)5s~^3P^o$ & 0 & 0.83069 & 0.83080 &-0.0001 \\ & 1 & 0.83090 & 0.83096 &-0.0001 \\ & 2 & 0.83117 & 0.83131 &-0.0001 \\ $3s^23p^3(^2P^o)4d~^3P^o$ & 2 & 0.85493 & 0.84642 & 0.0085 \\ & 1 & 0.85577 & 0.84689 & 0.0089 \\ & 0 & 0.85628 & & \\ $3s^23p^3(^2D^o)3d~^1P^o$ & 1 & 0.52030 & 0.52697 &-0.0067 \\ $3s^23p^3(^2P^o)4s~^1P^o$ & 1 & 0.63342 & 0.63907 &-0.0056 \\ $3s^23p^3(^2D^o)4d~^1P^o$ & 1 & 0.74478 & 0.74365 & 0.0011 \\ $3s^23p^3(^2P^o)3d~^1P^o$ & 1 & 0.78086 & 0.77554 & 0.0053 \\ $3s^23p^3(^2D^o)4d~^1P^o$ & 1 & 0.82316 & 0.81954 & 0.0036 \\ $3s^23p^3(^2P^o)5s~^1P^o$ & 1 & 0.83541 & 0.83540 & 0.0000 \\ $3s^23p^3(^4S^o)3d~^3D^o$ & 3 & 0.54799 & 0.54590 & 0.0021 \\ & 2 & 0.54804 & 0.54585 & 0.0022 \\ & 1 & 0.54808 & 0.54605 & 0.0020 \\ $3s^23p^3(^2D^o)4s~^3D^o$ & 1 & 0.57323 & 0.57741 &-0.0042 \\ & 2 & 0.57320 & 0.57749 &-0.0043 \\ & 3 & 0.57323 & 0.57767 &-0.0044 \\ $3s^23p^3(^2D^o)3d~^3D^o$ & 1 & 0.64563 & 0.64127 & 0.0044 \\ & 2 & 0.64630 & 0.64250 & 0.0038 \\ & 3 & 0.64717 & 0.64404 & 0.0031 \\ $3s^23p^3(^2P^o)3d~^3D^o$ & 3 & 0.69501 & 0.68656 & 0.0084 \\ & 2 & 0.69456 & 0.68810 & 0.0065 \\ & 1 & 0.69431 & 0.68862 & 0.0057 \\ $3s^23p^3(^4S^o)4d~^3D^o$ & 3 & 0.73720 & 0.73721 & 0.0000 \\ & 2 & 0.73795 & 0.73771 & 0.0002 \\ & 1 & 0.73847 & 0.73663 & 0.0018 \\ $3s^23p^3(^2D^o)5s~^3D^o$ & 1 & 0.76894 & 0.77693 &-0.0080 \\ & 2 & 0.76892 & 0.77702 &-0.0081 \\ & 3 & 0.76896 & 0.77721 &-0.0082 \\ $3s^23p^3(^4S^o)5d~^3D^o$ & 1 & 0.78244 & 0.77937 & 0.0031 \\ & 2 & 0.78224 & 0.77916 & 0.0031 \\ & 3 & 0.78195 & 0.77902 & 0.0029 \\ $3s^23p^3(^2D^o)4d~^3D^o$ & 1 & 0.80846 & 0.79639 & 0.0121 \\ & 2 & 0.80855 & 0.79655 & 0.0120 \\ & 3 & 0.80864 & 0.79670 & 0.0119 \\ $3s^23p^3(^4S^o)4s~^5S^o$ & 2 & 0.49022 & 0.49154 &-0.0013 \\ $3s^23p^3(^4S^o)5s~^5S^o$ & 2 & 0.69082 & 0.69363 &-0.0028 \\ $3s^23p^3(^4S^o)4s~^3S^o$ & 1 & 0.53010 & 0.51309 & 0.0170 \\ $3s^23p^3(^4S^o)5s~^3S^o$ & 1 & 0.69905 & 0.70001 &-0.0010 \\ \hline \end{tabular} \end{table} \clearpage \begin{table} \caption[]{The length ($f_L$) and velocity ($f_V$) values of oscillator strengths and length ($A_L$) value of transition probability for allowed transitions. Deb: calculted values of Deb et al. (2003)} \begin{tabular}{ccccccccc} \hline \multicolumn{1}{c}{Transition}& \multicolumn{1}{c}{$J$}& \multicolumn{1}{c}{$J'$}& \multicolumn{1}{c}{$\lambda$(\AA)}& \multicolumn{3}{c}{Present results}& \multicolumn{2}{c}{Deb}\\ & & & & $f_L$ & $f_V$ & $A_L$~$(s^{-1})$& $f_L$ & $f_V$ \\ \hline $3s^23p^4~^3P_J$ - $3s3p^5~^3P^o_{J'}$ & 2 & 2 & 1071.036 & 1.38(-2) & 1.60(-2) & 7.63(7) &1.11(-2) & 1.09(-2) \\ & 2 & 1 & 1063.831 & 4.61(-3) & 5.11(-3) & 4.31(7) &&\\ & 1 & 2 & 1079.080 & 7.72(-3) & 9.07(-3) & 2.53(7) &&\\ & 1 & 1 & 1071.767 & 4.53(-3) & 5.12(-3) & 2.51(7) &&\\ & 1 & 0 & 1067.944 & 6.10(-3) & 7.14(-3) & 1.02(8) &&\\ & 0 & 1 & 1075.229 & 1.83(-2) & 2.09(-2) & 3.36(7) &1.58(-2) & 1.68(-2) \\ $3s^23p^4~^3P_J$ - $3s^23p^3(^2P^o)4s~^3P^o_{J'}$ & 2 & 2 & 725.272 & 1.04(-1) & 1.08(-1) & 1.32(9) & 7.48(-2) & 7.07(-2) \\ & 2 & 1 & 725.657 & 3.62(-2) & 3.74(-2) & 7.61(8) & 2.39(-2) & 2.25(-2) \\ & 1 & 2 & 728.951 & 7.27(-2) & 7.47(-2) & 5.46(8) & 4.73(-2) & 4.53(-2) \\ & 1 & 1 & 729.341 & 3.31(-2) & 3.50(-2) & 4.14(8) & 2.50(-2) & 2.37(-2) \\ & 1 & 0 & 729.523 & 4.87(-2) & 5.08(-2) & 1.82(9) & & \\ & 0 & 1 & 730.942 & 1.60(-1) & 1.67(-1) & 6.65(8) & 1.17(-1) & 1.11(-1) \\ $3s^23p^4~^3P_J$ - $3s^23p^3(^2P^o)3d~^3P^o_{J'}$ & 2 & 2 & 684.862 & 5.24(-6) & 1.07(-5) & 7.57(4) & 4.32(-2) & 4.11(-2) \\ & 2 & 1 & 687.657 & 7.10(-6) & 2.18(-5) & 1.70(5) & 1.59(-2) & 1.52(-2) \\ & 1 & 2 & 688.142 & 2.50(-5) & 5.39(-5) & 2.15(5) & 3.37(-2) & 3.65(-2) \\ & 1 & 1 & 690.964 & 2.32(-6) & 9.33(-7) & 3.30(4) &&\\ & 1 & 0 & 692.402 & 3.12(-5) & 1.52(-5) & 1.33(6) & 2.06(-2) & 2.06(-2) \\ & 0 & 1 & 693.582 & 1.46(-4) & 2.38(-4) & 6.91(5) & 6.67(-2) & 7.29(-2) \\ $3s^23p^4~^3P_J$ - $3s^23p^3(^2D^o)3d~^3P^o_{J'}$ & 2 & 2 & 636.624 & 5.27(-1) & 5.20(-1) & 8.95(9) &&\\ & 2 & 1 & 634.257 & 1.76(-1) & 1.72(-1) & 5.00(9) &&\\ & 1 & 2 & 639.458 & 2.86(-1) & 2.82(-1) & 2.89(9) &&\\ & 1 & 1 & 637.069 & 1.77(-1) & 1.75(-1) & 3.00(9) &&\\ & 1 & 0 & 635.880 & 2.33(-1) & 2.29(-1) & 1.19(10) &&\\ & 0 & 1 & 639.219 & 6.87(-1) & 6.78(-1) & 3.87(9) &&\\ $3s^23p^4~^3P_J$ - $3s^23p^3(^2D^o)4d~^3P^o_{J'}$ & 2 & 2 & 562.368 & 2.10(-1) & 1.90(-1) & 4.51(9) &&\\ & 2 & 1 & 562.566 & 6.66(-2) & 6.02(-2) & 2.38(9) &&\\ & 1 & 2 & 564.578 & 1.10(-1) & 9.96(-2) & 1.41(9) &&\\ & 1 & 1 & 565.017 & 6.86(-2) & 6.26(-2) & 1.46(9) &&\\ & 1 & 0 & 564.972 & 8.62(-2) & 7.83(-2) & 5.51(9) &&\\ & 0 & 1 & 565.738 & 2.53(-1) & 2.29(-1) & 1.79(9) &&\\ $3s^23p^4~^3P_J$ - $3s^23p^3(^2P^o)5s~^3P^o_{J'}$ & 2 & 2 & 548.093 & 7.48(-3) & 7.93(-3) & 1.66(8) &&\\ & 2 & 1 & 548.322 & 1.49(-3) & 1.66(-3) & 5.50(7) &&\\ & 1 & 2 & 550.192 & 3.25(-3) & 3.59(-3) & 4.31(7) &&\\ & 1 & 1 & 550.423 & 1.66(-3) & 1.80(-3) & 3.65(7) &&\\ & 1 & 0 & 550.528 & 1.46(-3) & 1.67(-3) & 9.65(7) &&\\ & 0 & 1 & 551.335 & 5.13(-3) & 5.82(-3) & 3.76(7) &&\\ $3s^23p^4~^3P_J$ - $3s^23p^3(^2P^o)4d~^3P^o_{J'}$ & 2 & 2 & 538.308 & 7.30(-2) & 6.29(-2) & 1.72(9) &&\\ & 2 & 1 & 538.005 & 2.95(-2) & 2.54(-2) & 1.16(9)&& \\ & 1 & 2 & 540.333 & 4.27(-2) & 3.70(-2) & 5.19(8) &&\\ & 1 & 1 & 540.027 & 2.88(-2) & 2.50(-2) & 6.74(8)&& \\ & 1 & 0 & 540.027 & 4.27(-2) & 3.70(-2) & 3.00(9) &&\\ & 0 & 1 & 540.905 & 1.22(-1) & 1.06(-1) & 9.46(8) &&\\ $3s^23p^4~^3P_J$ - $3s^23p^3(^4S^o)3d~^3D^o_{J'}$ & 2 & 3 & 834.646 & 2.20(-2) & 1.94(-2) & 1.52(8) &&\\ & 2 & 2 & 834.722 & 4.42(-3) & 3.96(-3) & 4.27(7) &&\\ & 2 & 1 & 834.422 & 3.19(-4) & 2.88(-4) & 5.13(6) &&\\ & 1 & 2 & 839.600 & 1.98(-2) & 1.87(-2) & 1.14(8) & 2.00(-2) & 1.94(-2)\\ & 1 & 1 & 839.297 & 7.15(-3) & 6.47(-3) & 6.83(7) &&\\ & 0 & 1 & 841.419 & 2.70(-2) & 2.44(-2) & 8.57(7) &&\\ $3s^23p^4~^3P_J$ - $3s^23p^3(^2D^o)4s~^3D^o_{J'}$ & 2 & 3 & 788.741 & 1.26(-1) & 1.27(-1) & 9.53(8) & 1.56(-1) & 1.46(-1) \\ & 2 & 2 & 788.986 & 2.36(-2) & 2.39(-2) & 2.50(8) & 2.29(-2) & 2.29(-2) \\ & 2 & 1 & 789.100 & 1.63(-3) & 1.65(-3) & 2.86(7) &&\\ & 1 & 2 & 793.342 & 1.10(-1) & 1.11(-1) & 6.92(8) & 9.80(-2) & 9.92(-2) \\ & 1 & 1 & 793.457 & 3.79(-2) & 3.84(-2) & 3.97(8) &4.97(-2) & 4.59(-2) \\ & 0 & 1 & 795.354 & 1.46(-1) & 1.48(-1) & 5.08(8) & 1.74(-1) & 1.61(-1) \\ \hline \end{tabular} \end{table} \clearpage \begin{table} \caption[]{The length ($f_L$) and velocity ($f_V$) values of oscillator strengths and length ($A_L$) value of transition probability for allowed transitions. Deb: calculated values of Deb et al. (2003)} \begin{tabular}{ccccccccc} \hline \multicolumn{1}{c}{Transition}& \multicolumn{1}{c}{$J$}& \multicolumn{1}{c}{$J'$}& \multicolumn{1}{c}{$\lambda$(\AA)}& \multicolumn{3}{c}{Present results}& \multicolumn{2}{c}{Deb}\\ & & & & $f_L$ & $f_V$ & $A_L$~$(s^{-1})$& $f_L$ & $f_V$ \\ \hline $3s^23p^4~^3P_J$ - $3s^23p^3(^2D^o)3d~^3D^o_{J'}$ & 2 & 3 & 707.458 & 3.91(-1) & 3.54(-1) & 3.76(9) &&\\ & 2 & 2 & 709.162 & 6.50(-2) & 5.85(-2) & 8.73(8) &&\\ & 2 & 1 & 710.521 & 1.44(-1) & 9.68(-2) & 6.27(6) &&\\ & 1 & 2 & 712.679 & 3.31(-1) & 3.00(-1) & 2.64(9) &&\\ & 1 & 1 & 714.052 & 1.05(-1) & 9.46(-2) & 1.40(9) &&\\ & 0 & 1 & 715.587 & 4.23(-1) & 3.82(-1) & 1.87(9) &&\\ $3s^23p^4~^3P_J$ - $3s^23p^3(^2P^o)3d~^3D^o_{J'}$ & 2 & 3 & 663.643 & 9.81(-2) & 8.32(-2) & 1.09(9) &&\\ & 2 & 2 & 662.164 & 1.99(-2) & 1.66(-2) & 3.09(8) &&\\ & 2 & 1 & 661.659 & 1.42(-3) & 1.18(-3) & 3.68(7) &&\\ & 1 & 2 & 665.229 & 9.26(-2) & 7.78(-2) & 8.55(8) &&\\ & 1 & 1 & 664.720 & 3.33(-2) & 2.78(-2) & 5.12(8) &&\\ & 0 & 1 & 666.050 & 1.29(-1) & 1.07(-1) & 6.57(8) &&\\ $3s^23p^4~^3P_J$ - $3s^23p^3(^4S^o)4d~^3D^o_{J'}$ & 2 & 3 & 618.054 & 5.12(-1) & 5.21(-1) & 6.39(9) &&\\ & 2 & 2 & 617.629 & 9.59(-2) & 9.65(-2) & 1.68(9) &&\\ & 2 & 1 & 617.316 & 6.62(-3) & 6.60(-3) & 1.93(8) &&\\ & 1 & 2 & 620.296 & 4.56(-1) & 4.65(-1) & 4.75(9) &&\\ & 1 & 1 & 619.980 & 1.57(-1) & 1.59(-1) & 2.73(9) &&\\ & 0 & 1 & 621.137 & 6.10(-1) & 6.22(-1) & 3.52(9) &&\\ $3s^23p^4~^3P_J$ - $3s^23p^3(^2D^o)5s~^3D^o_{J'}$ & 2 & 3 & 586.244 & 1.78(-2) & 1.73(-2) & 2.42(8) &&\\ & 2 & 2 & 586.383 & 3.58(-3) & 3.44(-3) & 6.81(7) &&\\ & 2 & 1 & 586.453 & 2.57(-4) & 2.45(-4) & 8.15(6) &&\\ & 1 & 2 & 588.786 & 1.55(-2) & 1.51(-2) & 1.75(8) &&\\ & 1 & 1 & 588.856 & 5.61(-3) & 5.42(-3) & 1.06(8) &&\\ & 0 & 1 & 589.900 & 2.08(-2) & 2.03(-2) & 1.31(8) &&\\ $3s^23p^4~^3P_J$ - $3s^23p^3(^4S^o)5d~^3D^o_{J'}$ & 2 & 3 & 584.883 & 5.64(-2) & 6.13(-2) & 7.92(8) &&\\ & 2 & 2 & 584.772 & 1.08(-2) & 1.16(-2) & 2.12(8) &&\\ & 2 & 1 & 584.616 & 7.48(-4) & 8.01(-4) & 2.45(7) &&\\ & 1 & 2 & 587.162 & 5.45(-2) & 5.93(-2) & 6.39(8) &&\\ & 1 & 1 & 587.004 & 1.90(-2) & 2.05(-2) & 3.71(8) &&\\ & 0 & 1 & 588.041 & 7.64(-2) & 8.28(-2) & 4.96(8) &&\\ $3s^23p^4~^3P_J$ - $3s^23p^3(^2D^o)4d~^3D^o_{J'}$ & 2 & 3 & 571.903 & 2.12(-1) & 2.13(-1) & 3.18(9) &&\\ & 2 & 2 & 572.008 & 3.96(-2) & 3.94(-2) & 8.33(8) &&\\ & 2 & 1 & 572.121 & 2.71(-3) & 2.68(-3) & 9.51(7) &&\\ & 1 & 2 & 574.295 & 1.87(-1) & 1.89(-1) & 2.34(9) &&\\ & 1 & 1 & 574.409 & 6.42(-2) & 6.44(-2) & 1.34(9) &&\\ & 0 & 1 & 575.402 & 2.49(-1) & 2.52(-1) & 1.73(9) &&\\ $3s^23p^4~^3P_J$ - $3s^23p^3(^4S^o)4s~^3S^o_{J'}$ & 2 & 1 & 888.026 & 1.11(-1) & 9.98(-2) & 1.57(9) & 1.26(-1) & 1.11(-1) \\ & 1 & 1 & 893.548 & 1.08(-1) & 9.75(-2) & 9.04(8) & 1.23(-1) & 1.08(-1) \\ & 0 & 1 & 895.954 & 1.07(-1) & 9.61(-2) & 2.96(8) & 1.23(-1) & 1.07(-1) \\ $3s^23p^4~^1D_J$ - $3s^23p^3(^2D^o)3d~^1P^o_{J'}$ & 2 & 1 & 961.500 & 6.11(-3) & 7.16(-3) & 7.10(7) &&\\ $3s^23p^4~^1D_J$ - $3s^23p^3(^2P^o)4s~^1P^o_{J'}$ & 2 & 1 & 777.562 & 1.23(-1) & 1.21(-1) & 2.22(9) &&\\ $3s^23p^4~^1D_J$ - $3s^23p^3(^2D^o)4d~^1P^o_{J'}$ & 2 & 1 & 659.811 & 2.29(-1) & 2.16(-1) & 5.85(9) &&\\ $3s^23p^4~^1D_J$ - $3s^23p^3(^2P^o)3d~^1P^o_{J'}$ & 2 & 1 & 630.682 & 3.95(-5) & 3.32(-5) & 1.12(6) &&\\ $3s^23p^4~^1D_J$ - $3s3p^5~^1P^o_{J'}$ & 2 & 1 & 594.475 & 1.89(-1) & 1.80(-1) & 5.98(9) &&\\ $3s^23p^4~^1D_J$ - $3s^23p^3(^2P^o)5s~^1P^o_{J'}$ & 2 & 1 & 582.427 & 3.68(-2) & 3.47(-2) & 1.20(9) &&\\ $3s^23p^4~^1D_J$ - $3s^23p^3(^2P^o)4d~^1P^o_{J'}$ & 2 & 1 & 523.460 & 5.07(-2) & 4.43(-2) & 2.06(9) &&\\ $3s^23p^4~^1D_J$ - $3s^23p^3(^2D^o)4s~^1D^o_{J'}$ & 2 & 2 & 851.692 & 2.33(-1) & 2.22(-1) & 2.18(9) & 2.65(-1) & 2.41 (-1)\\ $3s^23p^4~^1D_J$ - $3s^23p^3(^2P^o)3d~^1D^o_{J'}$ & 2 & 2 & 787.580 & 7.74(-2) & 6.51(-2) & 1.19(9) &&\\ $3s^23p^4~^1D_J$ - $3s^23p^3(^2D^o)3d~^1D^o_{J'}$ & 2 & 2 & 682.476 & 4.99(-1) & 3.43(-1) & 1.00(10) &&\\ $3s^23p^4~^1S_J$ - $3s^23p^3(^2D^o)3d~^1P^o_{J'}$ & 0 & 1 & 961.500 & 6.11(-3) & 7.16(-3) & 7.10(7) &&\\ $3s^23p^4~^1S_J$ - $3s^23p^3(^2P^o)4s~^1P^o_{J'}$ & 0 & 1 & 889.817 & 1.73(-1) & 2.14(-1) & 4.77(8) &&\\ $3s^23p^4~^1S_J$ - $3s^23p^3(^2D^o)4d~^1P^o_{J'}$ & 0 & 1 & 738.912 & 3.35(-4) & 1.31(-4) & 1.38(6) &&\\ $3s^23p^4~^1S_J$ - $3s^23p^3(^2P^o)3d~^1P^o_{J'}$ & 0 & 1 & 702.573 & 1.10 & 1.20 & 5.07(9) &&\\ $3s^23p^4~^1S_J$ - $3s3p^5~^1P^o_{J'}$ & 0 & 1 & 657.915 & 1.03(-2) & 1.53(-2) & 5.38(7) &&\\ $3s^23p^4~^1S_J$ - $3s^23p^3(^2P^o)5s~^1P^o_{J'}$ & 0 & 1 & 643.207 & 1.37(-1) & 1.46(-1) & 7.39(8) &&\\ $3s^23p^4~^1S_J$ - $3s^23p^3(^2P^o)4d~^1P^o_{J'}$ & 0 & 1 & 569.900 & 2.14(-1) & 2.11(-1) & 1.46(9) &&\\ \hline \end{tabular} \end{table} \clearpage \begin{table} \caption[]{The length ($f_L$) and velocity ($f_V$) values of oscillator strengths and length ($A_L$) value of transition probability for intercombination transitions.} \begin{tabular}{ccccccc} \hline \multicolumn{1}{c}{Transition}& \multicolumn{1}{c}{$J$}& \multicolumn{1}{c}{$J'$}& \multicolumn{1}{c}{$\lambda$(\AA)}& \multicolumn{3}{c}{Present results}\\ & & & & $f_L$ & $f_V$ & $A_L$~$(s^{-1}$) \\ \hline $3s^23p^4~^3P_J$ - $3s^23p^3(^4S^o)4d~^5D^o_{J'}$ & 2 & 3 & 646.732 & 4.79(-3) & 3.59(-3) & 5.47(7) \\ & 2 & 2 & 646.743 & 7.22(-3) & 5.79(-3) & 1.15(8) \\ & 2 & 1 & 646.751 & 1.35(-3) & 1.15(-3) & 3.60(7) \\ & 1 & 2 & 649.667 & 1.75(-2) & 1.32(-2) & 1.67(8) \\ & 1 & 1 & 649.675 & 1.98(-2) & 1.55(-2) & 3.13(8) \\ & 0 & 1 & 650.946 & 5.66(-2) & 4.71(-2) & 2.98(8) \\ $3s^23p^4~^1D_J$ - $3s^23p^3(^2P^o)4s~^3P^o_{J'}$ & 2 & 2 & 792.231 & 1.99(-3) & 1.87(-3) & 2.09(7) \\ $3s^23p^4~^1D_J$ - $3s^23p^3(^2D^o)3d~^3P^o_{J'}$ & 2 & 2 & 687.640 & 3.54(-4) & 4.25(-4) & 5.13(6) \\ & 2 & 1 & 684.879 & 2.15(-4) & 2.40(-4) & 5.23(6) \\ $3s^23p^4~^1S_J$ - $3s^23p^3(^2P^o)4s~^3P^o_{J'}$ & 0 & 1 & 909.685 & 1.84(-4) & 2.08(-4) & 4.93(5) \\ $3s^23p^4~^1S_J$ - $3s^23p^3(^2D^o)3d~^3P^o_{J'}$ & 0 & 1 & 770.494 & 5.87(-4) & 7.39(-4) & 2.29(6) \\ $3s^23p^4~^1S_J$ - $3s^23p^3(^2D^o)4d~^3P^o_{J'}$ & 0 & 1 & 667.539 & 2.47(-4) & 2.80(-4) & 1.27(6) \\ $3s^23p^4~^1S_J$ - $3s^23p^3(^2P^o)4d~^3P^o_{J'}$ & 0 & 1 & 632.953 & 1.10(-4) & 1.21(-4) & 6.29(5) \\ $3s^23p^4~^3P_J$ - $3s^23p^3(^2D^o)3d~^1P^o_{J'}$ & 2 & 1 & 864.620 & 5.91(-4) & 3.96(-4) & 8.57(6) \\ & 1 & 1 & 869.854 & 7.34(-4) & 6.11(-4) & 6.32(6) \\ & 0 & 1 & 872.134 & 3.15(-3) & 2.88(-3) & 9.00(6) \\ $3s^23p^4~^3P_J$ - $3s^23p^3(^2P^o)4s~^1P^o_{J'}$ & 2 & 1 & 712.958 & 6.23(-4) & 4.61(-4) & 1.34(7) \\ & 1 & 1 & 716.514 & 2.56(-3) & 1.86(-3) & 3.27(7) \\ $3s^23p^4~^3P_J$ - $3s^23p^3(^2D^o)4d~^1P^o_{J'}$ & 2 & 1 & 612.699 & 9.72(-4) & 7.47(-4) & 2.89(7) \\ & 1 & 1 & 615.323 & 6.02(-3) & 4.03(-3) & 1.07(8) \\ & 0 & 1 & 616.463 & 2.95(-2) & 2.38(-2) & 1.74(8) \\ $3s^23p^4~^3P_J$ - $3s3p^5~^1P^o_{J'}$ & 2 & 1 & 555.960 & 6.05(-4) & 4.81(-4) & 2.20(7) \\ & 1 & 1 & 558.119 & 2.12(-4) & 1.69(-4) & 4.59(6) \\ $3s^23p^4~^3P_J$ - $3s^23p^3(^2P^o)5s~^1P^o_{J'}$ & 2 & 1 & 545.408 & 4.26(-4) & 3.25(-4) & 1.59(7) \\ & 0 & 1 & 548.388 & 3.43(-3) & 2.87(-3) & 2.54(7) \\ $3s^23p^4~^3P_J$ - $3s^23p^3(^2P^o)4d~^1P^o_{J'}$ & 2 & 1 & & 1.82(-2) & 1.63(-2) & 8.35(8) \\ & 1 & 1 & & 2.53(-2) & 2.14(-2) & 6.94(8) \\ & 0 & 1 & & 6.37(-2) & 4.59(-2) & 5.79(8) \\ $3s^23p^4~^1D_J$ - $3s^23p^3(^4S^o)4d~^3D^o_{J'}$ & 2 & 2 & 665.531 & 1.14(-4) & 1.34(-4) & 1.66(6) \\ $3s^23p^4~^1D_J$ - $3s^23p^3(^2D^o)4s~^3D^o_{J'}$ & 2 & 3 & 868.577 & 1.75(-4) & 1.76(-4) & 1.08(6) \\ $3s^23p^4~^1D_J$ - $3s^23p^3(^2D^o)3d~^3D^o_{J'}$ & 2 & 3 & 771.024 & 4.78(-4) & 4.86(-4) & 3.86(6) \\ $3s^23p^4~^1D_J$ - $3s^23p^3(^2P^o)3d~^3D^o_{J'}$ & 2 & 3 & 719.270 & 9.59(-5) & 1.06(-4) & 9.03(5) \\ $3s^23p^4~^1D_J$ - $3s^23p^3(^4S^o)5d~^3D^o_{J'}$ & 2 & 3 & 627.741 & 2.50(-4) & 2.82(-4) & 3.26(6) \\ $3s^23p^4~^1S_J$ - $3s^23p^3(^2D^o)4s~^3D^o_{J'}$ & 0 & 1 & 1011.647& 1.10(-4) & 2.02(-4) & 2.36(5) \\ $3s^23p^4~^1S_J$ - $3s^23p^3(^2D^o)3d~^3D^o_{J'}$ & 0 & 1 & 886.024 & 3.13(-4) & 5.01(-4) & 9.06(5) \\ $3s^23p^4~^1S_J$ - $3s^23p^3(^2P^o)3d~^3D^o_{J'}$ & 0 & 1 & 811.311 & 1.39(-4) & 1.26(-4) & 4.80(5) \\ $3s^23p^4~^1S_J$ - $3s^23p^3(^4S^o)4d~^3D^o_{J'}$ & 0 & 1 & 745.637 & 5.85(-4) & 7.18(-4) & 2.35(6) \\ $3s^23p^4~^1S_J$ - $3s^23p^3(^2D^o)4d~^3D^o_{J'}$ & 0 & 1 & 680.689 & 2.42(-4) & 3.01(-4) & 1.21(6) \\ \hline \end{tabular} \end{table} \end{document}