Table 3
Number of transitions in scandium spectra (first column) available from three sources: NIST database, Kurucz linelist (CD-ROM No. 23) and present calculations with FAC.
NIST E1 transitions | Kurucz | FAC E1 transitions | |||||||
obs | Ritz | only | gf | gf | gA/gAmax | gf e−5 E/I | |||
Ion | Totala | with gf | with gf | obs | >10-4 | >10-3 | >10-5 | >10-4 | |
|
|||||||||
Sc xxib | 8 | 0 | 0 | 0 | 780 | 732 | 606 | 588 | |
Sc xx | 37 | 0 | 37 | 0 | 2549 | 2194 | 1350 | 1493 | |
Sc xix | 79 | 29 | 47 | 3 | 790 | 754 | 701 | 684 | |
Sc xviii | 24 | 16 | 8 | 0 | 21 505 | 13 999 | 10 681 | 9449 | |
Sc xvii | 52 | 21 | 20 | 11 | 72398 | 39 927 | 26 906 | 23 070 | |
Sc xvi | 82 | 34 | 30 | 18 | 171 420 | 90 024 | 59 607 | 49 068 | |
Sc xv | 58 | 28 | 14 | 16 | 216 773 | 114 497 | 68 431 | 61 169 | |
Sc xiv | 63 | 33 | 21 | 9 | 158 608 | 85 919 | 49 826 | 46 103 | |
Sc xiii | 39 | 18 | 1 | 20 | 74 152 | 43 995 | 28 290 | 25 346 | |
Sc xii | 68 | 5 | 0 | 63 | 16 007 | 11 620 | 8084 | 7606 | |
Sc xi | 130 | 31 | 86 | 13 | 763 | 746 | 719 | 714 | |
Sc x | 99 | 25 | 4 | 70 | 20 974 | 15 774 | 14 387 | 11 723 | |
Sc ix | 35 | 15 | 0 | 20 | 95 | 67 043 | 43 752 | 39 634 | 29 692 |
Sc viii | 46 | 16 | 3 | 27 | 72 | 260 142 | 155 366 | 143 356 | 95 592 |
Sc vii | 53 | 15 | 5 | 33 | 124 | 408 929 | 236 975 | 207 634 | 133 874 |
Sc vi | 63 | 0 | 0 | 63 | 119 | 191 222 | 112 340 | 92 957 | 65 824 |
Sc v | 454 | 14 | 0 | 440 | 36 | 104 336 | 63 866 | 36 519 | 35 989 |
Sc iv | 407 | 4 | 0 | 403 | 1204 | 19 657 | 13 802 | 5921 | 8691 |
Sc iii | 133 | 79 | 18 | 36 | 226 | 735 | 682 | 656 | 615 |
total | 1930 | 383 | 294 | 1245 | 1876 | 1 808 783 | 1 046 964 | 796 265 | 607 290 |
Notes. The total number of dipolar electric transitions found in NIST (second column) is broken down into observed transitions given with gf values (third column), Ritz unobserved transitions with gf values (fourth column), and observed transitions without gf values (fifth column). All transitions listed by Kurucz have gf values (sixth column). The four last columns give the number of transitions calculated in this work and selected according to various criteria: lines with gf values greater than 10-4 and 10-3, lines with weighted transition probability gA greater than 10-5 relative to the maximum value in the ion. Finally (last column), transitions have been selected according to their gf values weighted by a Bolztmann factor e−E/kT, where E is the lower level excitation energy and the energy kT is one fifth of the ionization potential of the ion.
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