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Table 1

Parameters of the full set of lines for which 3D non-LTE effects are discussed.

Transition λair χexc. log gf σlog gf log(γrad.s−1) α
2p2 1D2 2p2 1S0 872.7121 1.264 − 8.165 0.05 − 0.070

2p.4p 1D2 505.2164 7.685 − 1.303 0.05 + 8.592 1041 0.2369
2p.4p 1P1 538.0335 7.685 − 1.616 0.05 + 8.589 1041 0.2369
                   
2p.3p 1P1 658.7606 8.537 − 1.003 0.05 + 7.979 1944 0.3176
                   
2p.3p 3D1 711.1467 8.640 − 1.085 0.05 + 7.431 1849 0.3135
                   
2p.3p 3D3 711.3177 8.647 − 0.773 0.05 + 7.431 1864 0.3141
                   
2p.3p 1S0 833.5141 7.685 − 0.437 0.03 + 8.630 690 0.2257
                   
2p.3p 3P2 906.1427 7.483 − 0.347 0.05 + 8.595 581 0.2343
                   
2p.3p 3P1 906.2481 7.480 − 0.455 0.05 + 8.595 580 0.2343
                   
2p.3p 3P1 907.8278 7.483 − 0.581 0.05 + 8.595 580 0.2343
                   
2p.3p 3P0 908.8503 7.483 − 0.430 0.05 + 8.595 580 0.2344
                   
2p.3p 3P2 909.4824 7.488 + 0.151 0.05 + 8.595 581 0.2343
                   
2p.3p 3P1 911.1800 7.488 − 0.297 0.05 + 8.595 580 0.2344
                   
2p.3p 1D2 940.5721 7.685 + 0.286 0.03 + 8.620 633 0.2271
                   
2p.3p 3S1 960.3027 7.480 − 0.896 0.05 + 8.586 562 0.2363
                   
2p.3p 3S1 962.0767 7.483 − 0.445 0.05 + 8.586 562 0.2363
                   
2p.3p 3S1 965.8423 7.488 − 0.280 0.05 + 8.586 562 0.2364
                   
2p.3p 1P1 1012.387 8.537 − 0.031 0.09 + 8.264 822 0.2740
                   
2p.3p 3D1 1068.534 7.480 − 0.272 0.05 + 8.578 534 0.2377
                   
2p.3p 3D1 1070.731 7.483 − 0.411 0.05 + 8.578 534 0.2377
                   
2p.3p 3D2 1072.952 7.488 − 0.420 0.05 + 8.578 535 0.2379
                   
2p.3p 3D1 1075.397 7.488 − 1.606 0.05 + 8.578 534 0.2378
                   
2p.3p 3D2 1177.753 8.643 − 0.520 0.05 + 7.760 748 0.2704
                   
2p.3p 3D2 1184.870 8.643 − 0.697 0.05 + 8.143 1387 0.2221
                   
2p.3p 3D1 1186.300 8.640 − 0.710 0.05 + 8.143 1380 0.2217
                   
2p.3p 3D2 1189.289 8.643 − 0.277 0.05 + 8.143 1381 0.2216
                   
2p.3p 3D3 1189.575 8.647 − 0.008 0.05 + 8.143 1388 0.2220
                   
2p.3p 3P0 1254.949 8.847 − 0.565 0.05 + 8.375 866 0.2935
                   
2p.3p 3P1 1256.212 8.848 − 0.522 0.05 + 8.375 867 0.2936
                   
2p.3p 3P1 1256.904 8.848 − 0.598 0.05 + 8.375 866 0.2935
                   
2p.3p 3 P 1 1258.158 8.848 − 0.536 0.05 + 8.375 865 0.2932
                   
2p.3p 1 D 2 1744.856 9.003 + 0.012 0.03 + 8.052 1491 0.2727
                   
2p.3p 1 S 0 2102.316 9.172 − 0.398 0.05 + 8.339 788 0.2804
                   
2p.3p 1 S 0 2290.654 9.172 − 0.217 0.05 + 8.086 1382 0.3353
                   
2p.4p 1 D 2 3085.412 9.736 + 0.097 0.05 + 8.393 920 0.2793
                   
2p.4p 1 P 1 3406.491 9.989 + 0.443 0.05 + 7.319 1653 0.2653

Notes. Nominal uncertainties in log gf were taken from NIST. For the permitted lines, broadening via elastic collisions with hydrogen atoms is represented using σ, the cross-section at the reference velocity of 104 m s−1, and α, the exponent such that the cross-section varies with velocity as vα (e.g. Anstee & O’Mara 1995).

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