Table 1
Spectra of Se in a Tokamak-Generated Plasma: Se svi to Se xxiv
Spectrum Wavelength (Å) Intensitya Earlier Measurementb Classification Se xvi (K-like) 101.559 2 3p 6 3d 2 D 3/2 –3p 5 3d 2
(
F
3
)
D
2
5
/
2
∘ 101.663 40 2 D 3/2 –
(
F
3
)
D
2
3
/
2
∘ 102.235 100 2 D 5/2 –
(
P
3
)
P
2
3
/
2
∘ 102.536 10 2 D 3/2 –
(
P
3
)
P
2
1
/
2
∘ 102.715 100 2 D 5/2 –
(
F
3
)
D
2
5
/
2
∘ 110.087 20 2 D 5/2 –
(
F
3
)
F
2
7
/
2
∘ 112.383 50 2 D3/2 –
(
F
3
)
F
2
5
/
2
∘ Se xvii (Ar-like) 105.841 400 3s 2 3p 6 1 S 0 –3s 2 3p 5 3d
P
1
1
∘ 131.001 20 1 S 0 –
D
3
1
∘ Se xviii (Cl-like) 107.004 2
3
s
2
3
p
5
P
2
3
/
2
∘
-
3
s
2
3
p
4 (3 P )3d 2 P 1/2 109.144 400
P
2
3
/
2
∘
- (3 P ) 2 D 5/2 109.873 50
P
2
3
/
2
∘
- (3 P ) 2 P 3/2 109.999 20
P
2
1
/
2
∘
- (3 P ) 2 D 3/2 111.977 10
P
2
3
/
2
∘
- (1 D ) 2 S 1/2 115.060 10
P
2
1
/
2
∘
- (3 P ) 2 P 1/2 116.459 10
P
2
3
/
2
∘
- (1 S ) 2 D 3/2 Se xix (S-like) 113.824 50 3s 2 3p 4 3 p 2 –3s 2 3p 3
(
P
2
)
3
d
D
3
3
∘ 113.998 100 3 P 2 –
(
D
2
)
P
3
2
∘ 114.126 20 1 D 2 –
(
D
2
)
F
1
3
∘ 116.255 5 1 D 2 –
(
D
2
)
D
1
2
∘ 117.364 8 3 P 1 –
(
P
2
)
D
3
2
∘ 118.568 5 1 S 0
(
P
2
)
P
1
1
∘ Se xx (P-like) 118.568 5
3
s
2
3
p
3
D
2
3
/
2
∘
-
3
s
2
3
p
2 (3 P )3d 2 F 5/2 119.026 100
D
2
5
/
2
∘
- (3 P ) 2 F 7/2 120.014 20
S
4
3
/
2
∘
- (3 P ) 4 P 3/2 121.211 10
S
4
3
/
2
∘
- (3 P ) 4 P 1/2 123.331 60
S
4
3
/
2
∘
- (3 P ) 4 P 5/2 124.143 30
P
2
3
/
2
∘
- (3 P ) 2 D 5/2 218.188 10
S
4
3
/
2
∘
-
3
s
3
p
4 4 P 5/2 Se xxi (Si-like) 118.295 3 3s 2 3p 2 3 P 2 –3s 2 3p 3d
F
1
3
∘ 124.620 2 3 P 1
P
3
1
∘ 125.352 20 3 P 0 –
D
3
1
∘ 125.623 2 \ 3 P 1 –
P
3
0
∘ 128.950 40 3 P 2 –
D
3
3
∘ 129.075 20 3 D 2 –
F
1
3
∘ 130.999 20 3 P 2
D
1
2
∘ 135.768 30 1 S 0
P
1
1
∘ 3 P 1
P
3
2
∘ 140.095 5 bl 3 P 2 –
P
3
2
∘ 144.344 2 1 D 2
D
1
2
∘ 159.828 10 3 P 2 –3s 3p 3
S
3
1
∘ Se xxii (Al-like) 131.612 100 0.66 HS
3
s
2
3
p
P
2
1
/
2
∘
-
3
s
2
3
d 2 D 3/2 143.642 200 0.65 HS
P
2
3
/
2
∘
- 2 D 5/2 145.741 10 0.80 HS
P
2
3
/
2
∘
- 2 D 3/2 147.733 20 0.63 HS
P
2
3
/
2
∘
-
3
s
3
p
2 2 P 3/2 150.322 20 0.34 HS
P
2
1
/
2
∘
- 2 S 1/2 165.765 100 0.64 HS
P
2
3
/
2
∘
- 2 P 3/2 168.917 30 cl 0.87 HS
P
2
1
/
2
∘
- 2 P l/2168.983 10 cl 9.06 HS
P
2
3
/
2
∘
- 2 S 1/2 194.502 10 0.44 HS
P
2
1
/
2
∘
- 2 D 3/2 216.967 10
P
2
3
/
2
∘
- 2 D 5/2 Se xxii (Mg-like) 144.344 2
3
s
3
p
P
3
1
∘
-
3
s
3
d 3 D 1 154.219 30 0.04 FH
P
3
2
∘
- 3 D 3 159.031 40 8.86 FH
P
1
1
∘
- 1 D 2 176.036 1000 5.92 FH 3s 2 1 S 0 –3s 3p
P
1
1
∘ 185.423 2
3
s
3
p
P
3
2
∘
-
3
p
2 3 P 2 191.030 2
P
3
1
∘
- 1 D 2 265.822 60 3s 1 S 0 –3s 3p
P
3
1
∘ Se xxiv (Na-like)c 156.448 5 0.468 KRC
3
p
P
2
1
/
2
∘
-
3
d 2 D 3/2 174.097 20 0.118 KRC
P
2
3
/
2
∘
- 2 D 5/2 201.010 500 0.07 KRC 3s 2 S 1/2 –3p
P
2
3
/
2
∘ 239.123 300 2 S 1/2
P
2
1
/
2
∘
a The symbols bl and cl signify perturbed line positions due to blended or close lines, respectively.
b HS, Ref.
3 ; FH, Ref.
16 ; and KRC, Ref.
23 .
c The present measurements of Se XXIV are included in Ref.
5 .
Table 2
Observed Energy Levels (in cm−1 ) of Se xvi to Se xxiv
Spectrum Configuration Term J Levela Leading Percentages Se xvi (K-like) 3s 2 3p 6 3d 2 D 3/2 0 5/2 11 080 (50) 3s 2 3p 5 3d 2 (3 F ) 2 F ∘5/2 889 810 (90) 54 43 (1 G ) 2 F ∘ 7/2 919 450 (90) 43 53 3s 2 3p 5 3d 2 (3 P ) 2 P ∘1/2 975 270 (90) 65 24 (1 S ) 2 P ∘ 3/2 989 220 (90) 72 17 (1 D ) 2 P ∘ 3s 2 3p 5 3d 2 (3 F ) 2 D ∘3/2 983 640 (90) 69 18 (1 D ) 2 D ∘ 5/2 984 650 (90) 69 17 Se xvii (Ar-like) 3s 2 3p 6 1 S ∘0 0 3s 2 3p 5 3d 1 P ∘1 944 810 (90) 98 2 3 D ∘3s 2 3p 5 d 1 763 350 (90) 98 2 1 P ∘Se xviii (Cl-like) 3s 2 3p 5 2 P ∘3/2 0 1/2 65 454 (13) 3s 2 3p 4 (1 S )3d 2 D 3/2 858 670 (80) 51 21 (1 D ) 2 D 3s 2 3p 4 (1 D )3d 2 S 1/2 893 040 (80) 67 20 3s 3p 6 2 S 3s 2 3p 4 (3 P )3d 2 P 3/2 910 140 (80) 47 26 (1 D ) 2 P 1/2 934 550 (80) 50 39 3s 2 3p 4 (3 P )3d 2 D 5/2 916 220 (80) 67 27 (1 D ) 2 D 3/2 974 550 (80) 56 19 (1 S ) 2 D Se xix (S-like) 3s 2 3p 4 3 P 2 0 86 14 1 D 0 T 40170(10)71 29 1 S 1 57 880 (10) 100 3s 2 3p 4 1 D 2 T 91932 (10)86 14 3 P 3s 2 3p 4 1 S 0 181 290 (50) 71 29 3 P 3s 2 3p 3 (2 D ∘)3d 3 P ∘2 877 210 (80) 69 10 (4 S ∘) 3 D ∘ 3s 2 3p 3 (2 P ∘)3d 3 D ∘3 878 550 (80) 44 26 (4 S ∘) 3 D ∘ 2 909 930 (80) 22 22 3s 2 Sp 3 (2 D ∘)3d 1 D ∘2 T 952 110 (80)45 17 (2 P ∘) 1 D ∘ 3s 2 3p 3 (2 D ∘)3d 1 P ∘3 T 968 160 (80)53 31 (2 P ∘) 1 P ∘ 3s 2 3p 3 (2 P ∘)3d 1 P ∘1 1024 690 (80) 72 10 (4 S ∘) 3 D ∘ Se xx (P-like) 3s 2 3p 3 4 S ∘3/2 0 77 17 2 P ∘3s 2 3p 3 2 D ∘3/2 64 687 (10) 70 17 4 S ∘5/2 88 067 (10) 100 3s 2 3p 3 2P ∘ 1/2 T 130 450 (35)100 3/2 T 174 720 (35)69 24 4 S ∘3s 3p 4 4 P 5/2 458 320 (20) 85 9 3p 2 (3 P )3d 4 P 3s 2 3p 2 (3 P )3d 4 P 5/2 810 830 (70) 78 8 3s 3p 4 4 P 1/2 825 010 (70) 56 23 3p 2 (1 D )3d 2 P 3/2 833 240 (70) 36 21 (3 P )3d 2 D 3s 2 3p 2 (3 P )3d 2 F 5/2 908 080 (70) 29 23 (1 D ) 2 F 7/2 928 220 (70) 63 34 3s 2 3p 2 (3 P )3d 2 D 5/2 T 980 240 (70)37 21 (1 S ) 2 D Se xxi (Si-like) 3s 2 3p 2 3 P 0 0 88 12 1 S 1 48 956 (10) 100 2 71695 (10) 65 35 3s 2 3p 2 1 D 2 142 271 (20) 65 35 3 P 3s 2 3p 2 1 S 0 T 205 300 (70)88 12 3 P 3s 3p 3 3 S ∘1 697 370 (40) 64 29 1 P °3s 2 3p 3d 3 P ∘2 785 500 (60) 49 20 3 D ∘0 844 990 (60) 94 6 3s 3p 3 3 P ∘ 1 851 400 (60) 65 24 3p 3d 3 D ∘ 3s 2 3p 3d 1 D ∘2 835 060 (60) 36 35 3 D ∘3s 2 3p 3d 3 D ∘1 797 750 (60) 60 20 3 P ×3 847 190 (60) 83 7 3s 3p 3 3 D ∘ 3s 2 3p 3d 1 F ∘3 917 030 (60) 92 6 3p 3d 3 D ∘ 3s 2 3p 3d 1 P ∘1 T 941 850 (60)80 12 3s 3p 3 1 P ∘ Se xxii (Al-like) 3s 2 3p 2 P ∘1/2 0 3/2 73 639 (10) 3s 3p 2 2 D 3/2 514 134 (30) 85 11 3s 2 3d 2 D 5/2 534 538 (30) 78 11 3s 3p 2 2 P 1/2 592 007 (30) 56 40 2 S 3/2 676 900 (30) 94 4 3s 2 3d 2 D 3s 3p 2 2 S 1/2 665 239 (40) 55 44 2 P 3s 2 3d 2 D 3/2 759 800 (50) 85 13 3s 3p 2 2 D 5/2 769 810 (50) 89 11 Se xxiii (Mg-like) 3s 2 1 S 0 0 98 2 3 P 2 1 S 3s 3p 3 P ∘0 [357 600] 100 1 376 192 (15) 96 4 1 P ∘2 434 532 (20) 100 3s 3p 1 P ∘1 568066 (30) 96 4 3 P ∘3p 2 3 P 0 [848 860] 89 11 1 [901 390] 100 2 973 839 (40) 71 21 1 D 3p 2 1 D 2 899 670 (30) 60 28 3 P 3s 3d 3 D 1 1068 980 (50) 100 2 [1074 370] 100 3 1082 960 (50) 100 3s 3d 1 D 2 1196 870 (50) 80 19 3 P 2 1 D Se xxiv (Na-like) 3s 2 S 1/2 0 3p 2 P ∘1/2 418 195 (20) 3/2 497 488 (20) 3d 2 D 3/2 1057 385 (40) 5/2 1071 880 (40)
a Uncertainties of level values are given in parentheses. Levels of Se
xxiii given in brackets are calculated from leagt-squares-fitted parameters.
Table 3
Fitted Radial Integrals (in cm−1 ) for the Configurations 3s 2 3p n and 3s 2 3p n −1 3d + 3s 3pn +1
Se xviii (n = 5) Se xix (n = 4) Se xx (n = 3) Se xxi (n = 2) Se xxii (n = 1) Se xxiii (n = 0) 3s 2 3p n F 2 (pp ) 177 190 (20) 180 220 (90) 180 170 (400) ζ (3p ) 43 636a 45 051 (3) 46 670 (20) 47 612 (60) 49 093a α 306 (1) 215 (5) 360 (40) 3s 3p n −1 3d F 2 (pp ) 159 620b 167 720b 184 140b F 2 (pd ) 178 630 (120) 176 270 (500) 184 890 (4000) 182 643 (40) G 1 (pd ) 178 090 (40) 183 500 (250) 215 320 (2000) 200 009 (30) G 3 (pd ) 117 200c 121 260c 142 850c 133 223c ζ (3p ) 44 240(20) 46 890 (80) 43 890 (700) 48 657 (7) ζ (3d ) 4 068b 4 138b 4 449b 4 410 (5) 5 347a α 250b 250b 250b 250b D 1 (pd )14 358 (60) 3s 3p n +1 F 2 (pp ) 185 452a G 1 (ps ) 219 978a 228 070 (100) ζ (3p )49 328a 51 270 (40) α 2506 R 1 (pp , sd ) 204 670 (50) 221 450b 218 130 (2000) 185 436 (50) 232 893a
a Exact fit of parameter to levels.
b Parameter value fixed in least-squares fit.
c Ratio of
G 1 to
G 3 fixed at HFR ratio.
Table 4
Fitted Radial Energy Integrals (in cm−1 ) for the Even-Parity Configurations of Mg-like Se (Se xxiii )
3s 2 3p 2 3s 3d Fitted/HFR F 2 (pp )182 100 (90) 0.853 G 2 (sd )168 860 (25) 0.973 ζ (3p )52 462a 1.046 ζ (3d )5586(4) 0.923 R 1 (ss , pp )230 525a 0.850 R 1 (sd , pp )206 168a 0.850
a Fixed at scaled HFR value. Scaling factor shown in last column.
Table 5
Ratio of Fitted Radial Integrals to HFR Values
Se xviii (3s 2 3p 5 ) Sexix (3s 2 3p 4 ) Se xx (3s 2 3p 3 ) Se xxi (3s 2 3p 2 ) Se xxii (3s 2 3p ) 3s 2 3p n F 2 (pp ) 0.869 0.873 0.862 ζ (3p ) 1.011 1.012 1.015 1.005 1.007 3s 2 3p n −1 3d F 2 (pp ) 0.794 0.824 0.894 F 2 (pd ) 0.891 0.866 0.897 0.874 G 1 (pd ) 0.795 0.814 0.950 0.877 G 3 (pd ) 0.795 0.814 0.950 0.877 ζ (3p ) 1.027 1.055 0.956 1.030 ζ (3d ) 0.831 0.809 0.832 0.790 0.866 3s 3p n +1 F 2 (pp ) 0.878 G 1 (sp ) 0.818 ζ (3p ) 1.012 R 1 ( pp , sd ) 0.871 0.936 0.916 0.773 0.965