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Non-relativistic energy values and wave functions of the K-shell excited resonance states 1s2s 22p 2, 1s2s2p 3, 1s2p 4 2, 4 L( L= S, P, D) in boron-like sulfur ion are calculated in the frame of multi-configuration saddle-point variation method. The electron correlation effects are considered by the expansion of configuration wave function. The wave functions are constructed and optimized by the orbital-spin angular momentum partial waves selected based on the rule of configuration interaction. To saturate the wave functional space and to improve the non-relativistic energy, the restricted variational method is used to calculate the restricted variational energy. Then, the mass polarization effect and relativistic correction are calculated by the perturbation theory. The quantum electrodynamics (QED) effect and higher-order relativistic correction are considered by the screened hydrogenic formula. Furthermore, the energy shift originating from the interaction between closed channel and open channel is also calculated. Finally, the accurate relativistic energy levels for these resonance states are obtained by adding the non-relativistic energy and all corrections. Using the optimized wave functions, the line strengths, oscillator strengths, radiative transition rates and transition wavelengths of electric-dipole transitions for the K-shell excited resonance states in boron-like sulfur ion are systematically calculated. In this work, the oscillator strengths and transition rates are given in the length, velocity, and acceleration gauges. The good agreement among the three gauges reflects that the calculated wave functions are reasonably accurate. The calculated radiative transition rates and transition wavelengths are compared with other theoretical data. Good agreement is obtained except the transition: 1s2s( 3S)2p 3 2P o→1s2 2s2p 2 2D. The deviation between our theoretical result and the MCDF theoretical value is about 46%, which needs further verifying. The Auger rates, Auger branching ratios, and Auger electron energy values of the important decay channels of the K-shell excited states are calculated by the saddle-point complex-rotation method. The calculated Auger rates and Auger electron energy values are also in good agreement with the corresponding reference data. For some K-shell states, the related energy levels and Auger branching ratios are reported for the first time. The present calculations results will provide valuable theoretical data for the calibration of spectral lines and Auger electron spectra in the relevant experiments. [1] [2] [3] [4] [5] [6] [7] [8] [9] [10] [11] [12] [13] [14] [15] [16] [17] [18] [19] [20] [21] [22] [23] [24] [25] [26] [27] [28] [29] [30] [31] -
共振态 ${E_{{\rm{nonrel}}}}/{\rm{a.u.}}$ ${E_{{\rm{total}}}}/{\rm{a.u.}}$ $ - {E_{{\rm{total}}}}/{\rm{eV}}$ ${E_{\rm{b}}} + \Delta {E_{{\rm{RV}}}}$ $\Delta {E_{{\rm{corr}}}}$ $\Delta {E_{\rm{S}}}$ 本文 SCUNC[21] 1s2s22p2 4P –229.35389 –0.64011 –0.00245 –229.99645 6258.52 1s2s22p2 2S –228.66774 –0.66777 –0.00174 –229.33725 6240.58 1s2s22p2 2P –228.81110 –0.66633 –0.00089 –229.47832 6244.42 1s2s22p2 2D –228.91613 –0.67942 0.00322 –229.59233 6247.52 1s2s(3S)2p3 4So –227.40768 –0.60823 0.00018 –228.01573 6204.62 1s2s(1S)2p3 4So –228.21123 –0.62298 0.00151 –228.83270 6226.85 1s2s(3S)2p3 4Po –228.00558 –0.62215 0.00106 –228.62667 6221.25 1s2s(3S)2p3 4Do –228.30315 –0.62288 –0.00017 –228.92620 6229.40 1s2s(3S)2p3 2So –226.86291 –0.62586 0.00070 –227.48807 6190.26 1s2s(3S)2p3 2Po –226.91669 –0.61114 0.00193 –227.52590 6191.29 1s2s(1S)2p3 2Po –227.28245 –0.61646 0.00620 –227.89271 6201.28 1s2s(3S)2p3 2Do –227.21472 –0.61330 0.00204 –227.82598 6199.46 1s2s(1S)2p3 2Do –227.56290 –0.62041 0.00280 –228.18051 6209.11 1s2p4 4P –226.53817 –0.55727 –0.00249 –227.09793 6179.65 6173.07 1s2p4 2S –225.47488 –0.56220 0.00072 –226.03636 6150.76 6145.67 1s2p4 2P –225.94003 –0.56493 0.00251 –226.50245 6163.44 6159.02 1s2p4 2D –226.07283 –0.56074 0.00279 –226.63078 6166.94 6163.51 偶宇称 奇宇称 S11+离子K壳层激发态共振态 共振态 本文 文献[19] 共振态 本文 文献[19] 1s2s22p2 4P1/2 6259.50 6265.62 1s2s(3S)2p3 4S3/2 6204.62 6207.16 1s2s22p2 4P3/2 6258.83 6264.85 1s2s(1S)2p3 4S3/2 6226.85 6229.68 1s2s22p2 4P5/2 6257.99 6264.05 1s2s(3S)2p3 4P1/2 6221.05 6223.62 1s2s22p2 2S1/2 6240.58 6243.03 1s2s(3S)2p3 4P3/2 6221.24 6223.52 1s2s22p2 2P1/2 6245.72 6248.94 1s2s(3S)2p3 4P5/2 6221.32 6223.54 1s2s22p2 2P3/2 6243.77 6247.23 1s2s(3S)2p3 4D1/2 6229.21 6231.96 1s2s22p2 2D3/2 6247.38 6251.29 1s2s(3S)2p3 4D3/2 6229.21 6232.01 1s2s22p2 2D5/2 6247.62 6251.38 1s2s(3S)2p3 4D5/2 6229.30 6232.00 1s2p4 4P1/2 6178.53 6180.77 1s2s(3S)2p3 4D7/2 6229.61 6231.85 1s2p4 4P3/2 6179.12 6181.26 1s2s(3S)2p3 2S1/2 6190.26 6192.27 1s2p4 4P5/2 6180.37 6182.44 1s2s(3S)2p3 2P1/2 6191.17 6193.98 1s2p4 2S1/2 6150.76 6152.75 1s2s(3S)2p3 2P3/2 6191.36 6193.65 1s2p4 2P1/2 6163.28 6165.34 1s2s(1S)2p3 2P1/2 6201.72 6204.18 1s2p4 2P3/2 6163.52 6166.42 1s2s(1S)2p3 2P3/2 6201.05 6206.82 1s2p4 2D3/2 6166.83 6169.56 1s2s(3S)2p3 2D3/2 6199.29 6199.03 1s2p4 2D5/2 6167.00 6169.69 1s2s(3S)2p3 2D5/2 6199.57 6202.14 1s2s(1S)2p3 2D3/2 6209.23 6212.93 1s2s(1S)2p3 2D5/2 6209.03 6212.33 S11+离子低位激发态 激发态 本文 NIST[31] 激发态 本文 NIST[31] 1s22s2p2 4P1/2 8617.38 8617.29 1s22s22p2P1/2 8641.58 8641.33 1s22s2p2 4P3/2 8616.83 8616.70 1s22s22p2P3/2 8639.78 8639.70 1s22s2p2 4P5/2 8615.98 8615.86 1s22p3 4S3/2 8565.71 8565.69 1s22s2p2 2S1/2 8586.78 8586.83 1s22p3 2P1/2 8545.44 8545.36 1s22s2p2 2P1/2 8584.06 8583.71 1s22p3 2P3/2 8545.42 8545.14 1s22s2p2 2P3/2 8582.99 8582.88 1s22p3 2D3/2 8555.97 8555.79 1s22s2p2 2D3/2 8598.49 8598.35 1s22p3 2D5/2 8555.74 8555.72 1s22s2p2 2D5/2 8598.39 8598.31 S12+离子低位激发态 激发态 本文 NIST[31] 激发态 本文 NIST[31] 1s22s2 1S0 8076.99 8076.93 1s22s2p1P1 8028.74 8028.63 1s22p2 1S0 7987.61 7987.44 1s22s2p3P0 8052.36 8052.23 1s22p2 1D2 8004.12 8003.85 1s22s2p3P1 8051.81 8051.70 1s22p2 3P0 8012.11 8012.06 1s22s2p3P2 8050.64 8050.50 1s22p2 3P1 8011.53 8011.37 1s22p2 3P2 8010.43 8010.37 初态 末态 S/a.u. ${A_{ik}}/{\rm{s}}^{-1}$ ${f_{ki}}$ λ/Å ${A_{\rm{l}}}$ ${A_{\rm{v}}}$ ${A_{\rm{a}}}$ 文献[17] ${f_{\rm{l}}}$ ${f_{\rm{v}}}$ ${f_{\rm{a}}}$ 本文 文献[17] 文献[21] 1s2s22p2 4P 1s22p3 4So 5.06[–4] 5.48[11] 5.32[11] 5.31[11] 5.09[11] 7.14[–3] 6.94[–3] 6.92[–3] 5.374 5.379 1s2p4 4P 1s22p3 4So 2.14[–2] 2.55[13] 2.65[13] 2.67[13] 2.57[13] 3.12[–1] 3.23 [–1] 3.26[–1] 5.196 5.193 5.203 1s2s22p2 2S 1s22s22p2Po 3.81[–3] 2.78[13] 2.82[13] 2.80[13] 2.93[13] 3.72[–2] 3.78[–2] 3.76[–2] 5.166 5.176 5.167 1s22p3 2Po 1.78[–4] 1.15[12] 1.15[12] 1.02[12] 9.87[11] 1.68[–3] 1.67[–3] 1.48[–3] 5.379 5.383 1s2s22p2 2P 1s22s22p2Po 3.26[–2] 7.88[13] 7.87[13] 7.84[13] 7.53[13] 3.18[–1] 3.18[–1] 3.17[–1] 5.175 5.176 1s22p3 2Po 1.80[–4] 3.87[11] 3.88[11] 3.99[12] 3.20[11] 1.69[–3] 1.69[–3] 1.74[–3] 5.388 5.392 1s22p3 2Do 6.30[–4] 1.37[12] 1.39[12] 1.40[12] 1.23[12] 3.56[–3] 3.61[–3] 3.64[–3] 5.364 5.368 1s2s22p2 2D 1s22s22p2Po 1.92[–2] 2.77[13] 2.67[13] 2.64[13] 2.71[13] 1.87[–1] 1.80[–1] 1.78[–1] 5.181 5.183 1s22p3 2Po 1.01[–4] 1.29[11] 1.28[11] 1.45[11] 1.35[11] 9.43[–4] 9.34[–4] 1.06[–3] 5.396 5.401 1s22p3 2Do 3.68[–4] 7.98[11] 8.18[11] 8.25[11] 7.74[11] 3.46[–3] 3.55[–3] 3.59[–3] 5.371 5.375 1s2p4 2S 1s22p3 2Po 7.14[–3] 5.17[13] 5.26[13] 5.28[13] 5.13[13] 6.96[–2] 7.08[–2] 7.11[–2] 5.178 5.175 5.191 1s2p4 2P 1s22p3 2Po 1.75[–2] 4.17[13] 4.26[13] 4.26[13] 3.97[13] 1.70[–1] 1.74[–1] 1.73[–1] 5.205 5.205 5.217 1s22p3 2Do 2.89[–2] 6.97[13] 6.80[13] 6.71[13] 6.17[13] 1.69[–1] 1.65[–1] 1.63[–1] 5.182 5.182 5.191 1s2p4 2D 1s22s22p2Po 2.58[–4] 4.09[11] 4.42[11] 4.14[11] 2.59[–3] 2.80[–3] 2.62[–3] 5.013 1s22p3 2Po 9.20[–3] 1.30[13] 1.32[13] 1.33[13] 1.32[13] 8.91[–2] 9.04[–2] 9.11[–2] 5.213 5.212 5.220 1s22p3 2Do 2.74[–2] 3.93[13] 4.10[13] 4.13[13] 4.02[13] 1.60[–1] 1.67[–1] 1.68[–1] 5.190 5.189 5.198 1s2s(1S)2p3 4So 1s22s2p2 4P 3.08[–2] 1.11[14] 1.09[14] 1.09[14] 1.09[14] 1.50[–1] 1.48[–1] 1.47[–1] 5.188 5.189 1s2s(3S)2p3 4So 1s22s2p2 4P 7.57[–4] 2.80[12] 2.90[12] 2.99[12] 2.28[12] 3.72[–3] 3.85[–3] 3.97[–3] 5.141 5.135 1s2s(3S)2p3 4Po 1s22s2p2 4P 2.33[–2] 2.81[13] 2.79[13] 2.80[13] 2.67[13] 1.14[–1] 1.13[–1] 1.13 [–1] 5.176 5.174 1s2s(3S)2p3 4Do 1s22s2p2 4P 3.89[–2] 2.79[13] 2.78[13] 2.77[13] 2.63[13] 1.89[–1] 1.88[–1] 1.88[–1] 5.194 5.192 1s2s(3S)2p3 2So 1s22s2p2 2P 1.57[–2] 1.13[14] 1.13[14] 1.13[14] 8.54[13] 1.53[–1] 1.52[–1] 1.52[–1] 5.181 5.180 1s2s(1S)2p3 2Po 1s22s2p2 2P 1.05[–3] 2.50[12] 2.78[12] 2.74[12] 2.53[12] 1.02[–2] 1.13[–2] 1.12[–2] 5.205 5.208 1s22s2p2 2D 1.71[–2] 4.14[13] 4.17[13] 4.14[13] 3.92[13] 1.00[–1] 1.01[–1] 1.00[–1] 5.172 5.173 1s2s(3S)2p3 2Po 1s22s2p2 2S 1.59[–3] 3.85[12] 3.93[12] 3.50[12] 3.55[12] 4.66[–2] 4.76[–2] 4.24[–2] 5.176 5.174 1s22s2p2 2P 1.00[–2] 2.42[13] 2.42[13] 2.30[13] 3.01[13] 9.79[–2] 9.79[–2] 9.31[–2] 5.183 5.183 1s22s2p2 2D 2.01[–3] 4.95[12] 4.92[12] 5.19[12] 3.38[12] 1.18[–2] 1.19[–2] 1.25[–2] 5.151 5.149 1s2s(1S)2p3 2Do 1s22s2p2 2P 1.85[–3] 2.60[12] 2.64[12] 2.64[12] 2.19[12] 1.79[–2] 1.81[–2] 1.81[–2] 5.222 5.225 1s22s2p2 2D 5.21[–2] 7.49[13] 7.54[13] 7.55[13] 7.13[13] 3.04[–1] 3.06[–1] 3.07[–1] 5.189 5.191 1s2s(3S)2p3 2Do 1s22s2p2 2P 1.70[–2] 2.43[13] 2.49[13] 2.50[13] 2.40[13] 1.65[–1] 1.69[–1] 1.70[–1] 5.201 5.201 1s22s2p2 2D 5.16[–3] 7.51[12] 7.72[12] 7.83[12] 7.84[12] 3.02[–2] 3.11[–2] 3.15[–2] 5.168 5.166 俄歇跃迁通道 俄歇跃迁率/s–1 BR/% 俄歇跃迁通道 俄歇跃迁率/s–1 BR(%) 本文 文献[17] 本文 文献[17] 1s2s22p2 2S →1s22s2 1S 5.05[13] 8.33[13] 23.3 1s2s(1S)2p3 2Po→1s22s2 1S 6.63[11] 2.33[11] 0.3 2S →1s22s2p1Po 6.35[13] 6.02[13] 29.3 2Po→1s22s2p1Po 1.18[12] 1.46[13] 0.5 2S →1s22s2p3Po 1.61[13] 2.06[13] 7.4 2Po→1s22s2p3Po 1.29[14] 1.22[14] 59.6 2S →1s22p2 1S 7.10[13] 7.85[13] 32.8 2Po→1s22p2 1S 6.50[12] 5.20[12] 3.0 2S →1s22p2 1D 1.53[13] 1.48[13] 7.1 2Po→1s22p2 1D 5.25[12] 9.54[12] 2.4 2P→1s22s2p1Po 1.82[13] 2.55[13] 14.7 2Po→1s22p2 3P 7.40[13] 7.54[13] 34.2 2P→1s22s2p3Po 1.05[13] 7.34[12] 8.5 2Do→1s22s2p1Po 7.30[12] 8.82[12] 2.8 2P→1s22p2 1D2 1.97[10] 7.42[12] 0 2Do→1s22s2p3Po 1.74[14] 1.74[14] 66.1 2P→1s22p2 3P 9.50[13] 8.68[13] 76.8 2Do→1s22p2 1D 9.55[12] 1.40[13] 3.6 2D→1s22s2 1S 1.24[14] 1.14[14] 40.3 2Do→1s22p2 3P 7.25[13] 7.66[13] 27.5 2D→1s22s2p1Po 6.80[13] 6.42[13] 22.1 4So→1s22p2 3P 3.85[13] 3.88[13] 100 2D→1s22s2p3Po 1.72[13] 2.26[13] 5.6 1s2s(3S)2p3 2So→1s22p2 3P 6.55[13] 4.35[13] 100 2D→1s22p2 1S 3.43[12] 2.82[12] 1.1 2Po→1s22s2 1S 4.33[12] 2.67[12] 1.6 2D→1s22p2 1D 9.15[13] 9.22[13] 29.8 2Po→1s22s2p1Po 1.28[14] 1.18[14] 46.9 2D→1s22p2 3P 3.37[12] 4.47[12] 1.1 2Po→1s22s2p3Po 5.40[12] 7.38[12] 2.0 4P→1s22s2p3Po 1.10[14] 1.18[14] 54.3 2Po→1s22p2 1S 4.54[13] 4.68[13] 16.6 4P→1s22p2 3P 9.25[13] 9.48[13] 45.7 2Po→1s22p2 1D 6.40[13] 6.23[13] 23.4 1s2p4 2S →1s22s2 1S 2.75[12] 3.04[11] 0.6 2Po→1s22p2 3P 2.58[13] 3.47[13] 9.5 2S →1s22s2p1Po 4.15[12] 4.73[12] 1.0 2Do→1s22s2p1Po 1.76[14] 1.71[14] 54.5 2S →1s22s2p3Po 8.57[11] 1.48[12] 0.2 2Do→1s22s2p3Po 6.85[12] 1.16[13] 2.1 2S →1s22p2 1S 2.43[14] 3.66[13] 56.3 2Do→1s22p2 1D 1.18[14] 1.19[14] 36.5 2S →1s22p2 1D 1.81[14] 1.87[14] 41.9 2Do→1s22p2 3P 2.22[13] 1.99[13] 6.9 2P→1s22s2p1Po 2.73[11] 5.19[11] 0.1 4So→1s22p2 3P 1.92[14] 2.02[14] 100 2P→1s22s2p3Po 2.38[11] 1.86[11] 0.1 4Po→1s22s2p3Po 1.35[14] 1.38[14] 88.9 2P→1s22p2 1D2 6.95[10] 2.06[13] 0 4Po→1s22p2 3P 1.68[13] 1.45[13] 11.1 2P→1s22p2 3P 2.15[14] 1.90[14] 99.8 4Do→1s22s2p3Po 1.84[14] 1.84[14] 90.4 2D→1s22s2 1S 2.95[12] 7.35[9] 1.0 4Do→1s22p2 3P 1.96[13] 1.41[13] 9.6 2D→1s22s2p1Po 1.35[12] 1.38[12] 0.5 2D→1s22s2p3Po 2.73[11] 4.54[11] 0.1 2D→1s22p2 1S 1.25[13] 4.09[13] 4.2 2D→1s22p2 1D 2.68[14] 2.74[14] 90.6 2D→1s22p2 3P 1.05[13] 1.26[13] 3.6 4P→1s22s2p3Po 1.96[12] 2.50[12] 0.9 4P→1s22p2 3P 2.08[14] 2.09[14] 99.1 跃迁通道 本文 文献[17] 跃迁通道 本文 文献[17] 1s2s22p2 2S1/2 1s22s2 1S0 1836.41 1837.80 1s2s(3S)2p3 2S1/2 1s22p2 3P0 1821.85 1825.18 1s22s2p1P1 1788.16 1787.75 1s22p2 3P1 1821.27 1824.50 1s22s2p3P0 1811.78 1812.97 1s22p2 3P2 1820.17 1823.49 1s22s2p3P1 1811.23 1812.44 1s2s(3S)2p3 2P1/2 1s22s2 1S0 1885.82 1888.35 1s22s2p3P2 1810.06 1811.23 1s22s2p1P0 1837.57 1838.30 1s22p2 1S0 1747.03 1746.35 1s22s2p3P1 1861.19 1863.52 1s22p2 1D2 1763.54 1763.33 1s22s2p3P2 1860.64 1862.99 1s2s22p2 2P1/2 1s22s2p1P1 1783.02 1782.25 1s22s2p3P3 1859.47 1861.78 1s22s2p3P0 1806.64 1807.47 1s22p2 1S0 1796.44 1796.90 1s22s2p3P1 1806.09 1806.94 1s22p2 1D2 1812.95 1813.88 1s22s2p3P2 1804.92 1805.74 1s22p2 3P0 1820.94 1823.09 1s22p2 1D2 1758.40 1757.84 1s22p2 3P1 1820.36 1822.41 1s22p2 3P0 1766.39 1767.05 1s22p2 3P2 1819.26 1821.40 1s22p2 3P1 1765.81 1766.37 1s2s(3S)2p3 2P3/2 1s22s2 1S0 1885.63 1888.87 1s22p2 3P2 1764.71 1765.36 1s22s2p1P0 1837.38 1838.83 1s2s22p2 2P3/2 1s22s2p1P1 1784.97 1784.03 1s22s2p3P1 1861.00 1864.05 1s22s2p3P0 1808.59 1809.25 1s22s2p3P2 1860.45 1863.51 1s22s2p3P1 1808.04 1808.72 1s22s2p3P3 1859.28 1862.31 1s22s2p3P2 1806.87 1807.52 1s22p2 1S0 1796.25 1797.43 1s22p2 1D2 1760.35 1759.62 1s22p2 1D2 1812.76 1814.41 1s22p2 3P0 1768.34 1768.83 1s22p2 3P0 1820.75 1823.62 1s22p2 3P1 1767.76 1768.15 1s22p2 3P1 1820.17 1822.94 1s22p2 3P2 1766.66 1767.14 1s22p2 3P2 1819.07 1821.93 1s2s22p2 2D3/2 1s22s2 1S0 1829.61 1830.38 1s2s(1S)2p3 2P1/2 1s22s2 1S0 1875.27 1877.33 1s22s2p1P1 1781.36 1780.34 1s22s2p1P0 1827.02 1827.28 1s22s2p3P0 1804.98 1805.56 1s22s2p3P1 1850.64 1852.50 1s22s2p3P1 1804.43 1805.02 1s22s2p3P2 1850.09 1851.97 1s22s2p3P2 1803.26 1803.82 1s22s2p3P3 1848.92 1850.77 1s22p2 1S0 1740.23 1738.94 1s22p2 1S0 1785.89 1785.88 1s22p2 1D2 1756.74 1755.92 1s22p2 1D2 1802.40 1802.87 1s22p2 3P0 1764.73 1765.13 1s22p2 3P0 1810.39 1812.08 1s22p2 3P1 1764.15 1764.45 1s22p2 3P1 1809.81 1811.40 1s22p2 3P2 1763.05 1763.44 1s22p2 3P2 1808.71 1810.39 1s2s22p2 2D5/2 1s22s2 1S0 1829.37 1830.33 1s2s(1S)2p3 2P3/2 1s22s2 1S0 1875.94 1877.26 1s22s2p1P1 1781.12 1780.29 1s22s2p1P0 1827.69 1827.21 1s22s2p3P0 1804.74 1805.51 1s22s2p3P1 1851.31 1852.43 1s22s2p3P1 1804.19 1804.97 1s22s2p3P2 1850.76 1851.90 1s22s2p3P2 1803.02 1803.77 1s22s2p3P3 1849.59 1850.70 1s22p2 1S0 1739.99 1738.89 1s22p2 1S0 1786.56 1785.81 1s22p2 1D2 1756.50 1755.87 1s22p2 1D2 1803.07 1802.80 1s22p2 3P0 1764.49 1765.08 1s22p2 3P0 1811.06 1812.01 1s22p2 3P1 1763.91 1764.40 1s22p2 3P1 1810.48 1811.33 1s22p2 3P2 1762.81 1763.39 1s22p2 3P2 1809.38 1810.32 1s2p4 2S1/2 1s22s2 1S0 1926.23 1930.57 1s2s(3S)2p3 2D3/2 1s22s2p1P0 1829.45 1831.14 1s22s2p1P1 1877.98 1880.52 1s22s2p3P0 1853.07 1856.36 1s22s2p3P0 1901.60 1905.75 1s22s2p3P1 1852.52 1855.83 1s22s2p3P1 1901.05 1905.21 1s22s2p3P2 1851.35 1854.62 1s22s2p3P2 1899.88 1904.01 1s22p2 1D2 1804.83 1806.72 1s22p2 1S0 1836.85 1839.13 1s22p2 3P0 1812.82 1815.93 1s22p2 1D2 1853.36 1856.11 1s22p2 3P1 1812.24 1815.25 1s2p4 2P1/2 1s22s2p1P1 1865.46 1867.17 1s22p2 3P2 1811.14 1814.24 1s22s2p3P0 1889.08 1892.39 1s2s(3S)2p3 2D5/2 1s22s2p1P0 1829.17 1830.60 1s22s2p3P1 1888.53 1891.86 1s22s2p3P0 1852.79 1855.82 1s22s2p3P2 1887.36 1890.66 1s22s2p3P1 1852.24 1855.28 1s22p2 1D2 1840.84 1842.76 1s22s2p3P2 1851.07 1854.08 1s22p2 3P0 1848.83 1851.97 1s22p2 1D2 1804.55 1806.18 1s22p2 3P1 1848.25 1851.29 1s22p2 3P0 1812.54 1815.39 1s22p2 3P2 1847.15 1850.28 1s22p2 3P1 1811.96 1814.71 1s2p4 2P3/2 1s22s2p1P1 1865.22 1866.27 1s22p2 3P2 1810.86 1813.70 1s22s2p3P0 1888.84 1891.50 1s2s(1S)2p3 2D3/2 1s22s2p1P0 1819.51 1819.23 1s22s2p3P1 1888.29 1890.96 1s22s2p3P0 1843.13 1844.45 1s22s2p3P2 1887.12 1889.76 1s22s2p3P1 1842.58 1843.92 1s22p2 1D2 1840.60 1841.86 1s22s2p3P2 1841.41 1842.71 1s22p2 3P0 1848.59 1851.07 1s22p2 1D2 1794.89 1794.81 1s22p2 3P1 1848.01 1850.39 1s22p2 3P0 1802.88 1804.02 1s22p2 3P2 1846.91 1849.38 1s22p2 3P1 1802.30 1803.35 1s2p4 2D3/2 1s22s2 1S0 1910.16 1913.47 1s22p2 3P2 1801.20 1802.33 1s22s2p1P1 1861.91 1863.42 1s2s(1S)2p3 2D5/2 1s22s2p1P0 1819.71 1819.38 1s22s2p3P0 1885.53 1888.64 1s22s2p3P0 1843.33 1844.60 1s22s2p3P1 1884.98 1888.11 1s22s2p3P1 1842.78 1844.07 1s22s2p3P2 1883.81 1886.91 1s22s2p3P2 1841.61 1842.86 1s22p2 1S0 1820.78 1822.02 1s22p2 1D2 1795.09 1794.96 1s22p2 1D2 1837.29 1839.01 1s22p2 3P0 1803.08 1804.17 1s22p2 3P0 1845.28 1848.22 1s22p2 3P1 1802.50 1803.50 1s22p2 3P1 1844.70 1847.54 1s22p2 3P2 1801.40 1802.49 1s22p2 3P2 1843.60 1846.53 1s2s(3S)2p3 4S3/2 1s22p2 3P0 1807.49 1810.50 1s2p4 2D5/2 1s22s2 1S0 1909.99 1913.40 1s22p2 3P1 1806.91 1809.82 1s22s2p1P1 1861.74 1863.35 1s22p2 3P2 1805.81 1808.81 1s22s2p3P0 1885.36 1888.57 1s2s(1S)2p3 4S3/2 1s22p2 3P0 1785.26 1785.14 1s22s2p3P1 1884.81 1888.04 1s22p2 3P1 1784.68 1784.46 1s22s2p3P2 1883.64 1886.84 1s22p2 3P2 1783.58 1783.45 1s22p2 1S0 1820.61 1821.95 1s2s(3S)2p3 4P1/2 1s22s2p3P0 1831.31 1832.66 1s22p2 1D2 1837.12 1838.94 1s22s2p3P1 1830.76 1832.13 1s22p2 3P0 1845.11 1848.15 1s22s2p3P2 1829.59 1830.93 1s22p2 3P1 1844.53 1847.47 1s22p2 3P0 1791.06 1792.24 1s22p2 3P2 1843.43 1846.46 1s22p2 3P1 1790.48 1791.56 1s2s22p2 4P1/2 1s22s2p3P0 1792.86 1791.05 1s22p2 3P2 1789.38 1790.55 1s22s2p3P1 1792.31 1790.51 1s2s(3S)2p3 4P3/2 1s22s2p3P0 1831.12 1832.56 1s22s2p3P2 1791.14 1789.31 1s22s2p3P1 1830.57 1832.03 1s22p2 3P0 1752.61 1750.62 1s22s2p3P2 1829.40 1830.83 1s22p2 3P1 1752.03 1749.94 1s22p2 3P0 1790.87 1792.14 1s22p2 3P2 1750.93 1748.93 1s22p2 3P1 1790.29 1791.46 1s2s22p2 4P3/2 1s22s2p3P0 1793.53 1791.83 1s22p2 3P2 1789.19 1790.45 1s22s2p3P1 1792.98 1791.30 1s2s(3S)2p3 4P5/2 1s22s2p3P0 1831.04 1832.48 1s22s2p3P2 1791.81 1790.09 1s22s2p3P1 1830.49 1831.95 1s22p2 3P0 1753.28 1751.40 1s22s2p3P2 1829.32 1830.75 1s22p2 3P1 1752.70 1750.72 1s22p2 3P0 1790.79 1792.06 1s22p2 3P2 1751.60 1749.71 1s22p2 3P1 1790.21 1791.38 1s2s22p2 4P5/2 1s22s2p3P0 1794.37 1792.66 1s22p2 3P2 1789.11 1790.37 1s22s2p3P1 1793.82 1792.13 1s2s(3S)2p3 4D1/2 1s22s2p3P0 1823.15 1824.54 1s22s2p3P2 1792.65 1790.92 1s22s2p3P1 1822.60 1824.01 1s22p2 3P0 1754.12 1752.23 1s22s2p3P2 1821.43 1822.80 1s22p2 3P1 1753.54 1751.55 1s22p2 3P0 1782.90 1784.11 1s22p2 3P2 1752.44 1750.54 1s22p2 3P1 1782.32 1783.43 1s2p4 4P1/2 1s22s2p3P0 1873.83 1876.31 1s22p2 3P2 1781.22 1782.42 1s22s2p3P1 1873.28 1875.78 1s2s(3S)2p3 4D3/2 1s22s2p3P0 1823.15 1824.49 1s22s2p3P2 1872.11 1874.57 1s22s2p3P1 1822.60 1823.96 1s22p2 3P0 1833.58 1835.88 1s22s2p3P2 1821.43 1822.75 1s22p2 3P1 1833.00 1835.20 1s22p2 3P0 1782.90 1784.06 1s22p2 3P2 1831.90 1834.19 1s22p2 3P1 1782.32 1783.39 1s2p4 4P3/2 1s22s2p3P0 1873.24 1875.77 1s22p2 3P2 1781.22 1782.38 1s22s2p3P1 1872.69 1875.24 1s2s(3S)2p3 4D5/2 1s22s2p3P0 1823.06 1824.41 1s22s2p3P2 1871.52 1874.03 1s22s2p3P1 1822.51 1823.88 1s22p2 3P0 1832.99 1835.34 1s22s2p3P2 1821.34 1822.67 1s22p2 3P1 1832.41 1834.66 1s22p2 3P0 1782.81 1783.98 1s22p2 3P2 1831.31 1833.65 1s22p2 3P1 1782.23 1783.30 1s2p4 4P5/2 1s22s2p3P0 1871.99 1874.50 1s22p2 3P2 1781.13 1782.29 1s22s2p3P1 1871.44 1873.96 1s2s(3S)2p3 4D7/2 1s22s2p3P1 1822.20 1823.70 1s22s2p3P2 1870.27 1872.76 1s22s2p3P2 1821.03 1822.50 1s22p2 3P0 1831.74 1834.07 1s22p2 3P1 1781.92 1783.13 1s22p2 3P1 1831.16 1833.39 1s22p2 3P2 1780.82 1782.12 1s22p2 3P2 1830.06 1832.38 -
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