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i-j | Transition | Int | Int | (Å) | (Å) | (Å) | (Å) |
3-29 | 2s22p53s 1P1-2p63s 1S0 | 0.38 | 0.19 | 89.760 | 87.52 | 87.319 | 89.79 |
5-56 | 2s22p53s 3P1-2s22p54p 1S0 | 0.15 | 46.307 | 46.19 | - | - | |
5-29 | 2s22p53s 3P1-2p63s 1S0 | 0.23 | 0.11 | 98.249 | 95.78 | 95.317 | 98.28 |
3-47 | 2s22p53s 1P1-2s22p54p 3P0 | 46.300 | 46.12 | - | - | ||
8-53 | 2s22p53p 3D3-2s22p54d 3F4 | 0.33 | 50.260 | 50.32 | 50.280 | - | |
22-37 | 2s22p53d 3D3-2p63d 1D2 | 0.11 | 0.11 | 92.283 | 90.34 | - | 92.35 |
2-44 | 2s22p53s 3P2-2s22p54p 3D3 | 0.16 | 46.400 | 46.64 | - | - | |
33-119 | 2p63p 1P1-2p64s 1S0 | 57.710 | 57.79 | - | - | ||
33-135 | 2p63p 1P1-2p64d 1D2 | 50.690 | 50.75 | - | - | ||
26-37 | 2s22p53d 1F3-2p63d 1D2 | 100.640 | 98.53 | - | 100.71 | ||
20-37 | 2s22p53d 3F3-2p63d 1D2 | 90.401 | 88.51 | - | 90.47 | ||
3-83 | 2s22p53s 1P1-2s22p55p 1S0 | - | 33.73 | - | - | ||
14-70 | 2s22p53p 1D2-2s22p54d 1F3 | 0.14 | - | 50.46 | - | - | |
13-69 | 2s22p53p 3P1-2s22p54d 3D2 | 0.11 | - | 50.44 | - | - | |
27-56 | 2s22p53d 1P1-2s22p54p 1S0 | 68.510 | 68.66 | - | - | ||
7-55 | 2s22p53p 3D2-2s22p54d 3F3 | 0.18 | 49.870 | 49.93 | 49.897 | - | |
19-36 | 2s22p53d 3F4-2p63d 3D3 | 0.25 | - | 91.29 | - | 93.20 | |
2-28 | 2s22p53s 3P2-2p63s 3S1 | 0.21 | - | 90.52 | - | 92.50 | |
21-37 | 2s22p53d 1D2-2p63d 1D2 | 91.550 | 89.60 | - | 91.62 | ||
8-32 | 2s22p53p 3D3-2p63p 3P2 | 0.27 | - | 90.40 | - | 92.40 | |
6-52 | 2s22p53p 3S1-2s22p54d 3P1 | 49.456 | 49.38 | 49.443 | - | ||
10-54 | 2s22p53p 3P2-2s22p54d 3P2 | - | 50.89 | - | - | ||
23-47 | 2s22p53d 3D1-2s22p54p 3P0 | 67.918 | 67.78 | - | - | ||
9-57 | 2s22p53p 1P1-2s22p54d 1D2 | - | 50.37 | 49.805 | - | ||
20-35 | 2s22p53d 3F3-2p63d 3D2 | 0.11 | - | 92.03 | - | 93.91 | |
8-38 | 2s22p53p 3D3-2s22p54s 3P2 | 57.320 | 57.40 | 57.331 | - | ||
14-42 | 2s22p53p 1D2-2s22p54s 3P1 | 57.536 | 57.68 | 57.646 | - | ||
11-59 | 2s22p53p 3P0-2s22p54d 3D1 | 51.247 | 51.29 | 51.236 | - | ||
25-37 | 2s22p53d 3D2-2p63d 1D2 | 100.211 | 98.06 | - | 100.29 | ||
24-37 | 2s22p53d 3F2-2p63d 1D2 | 99.553 | 97.45 | - | 99.63 | ||
9-59 | 2s22p53p 1P1-2s22p54d 3D1 | 49.750 | 49.75 | 49.748 | - | ||
15-71 | 2s22p53p 1S0-2s22p54d 1P1 | 52.780 | 53.25 | 52.754 | - | ||
19-62 | 2s22p53d 3F4-2s22p54f 3G5 | 0.69 | 58.760 | 58.93 | 58.783 | - | |
7-57 | 2s22p53p 3D2-2s22p54d 1D2 | - | 49.80 | 49.261 | - | ||
21-34 | 2s22p53d 1D2-2p63d 3D1 | - | 93.34 | - | 95.25 | ||
25-74 | 2s22p53d 3D2-2s22p54f 3D3 | 0.25 | 58.980 | 59.23 | 59.240 | - | |
17-63 | 2s22p53d 3P1-2s22p54f 3D2 | 0.11 | - | 58.33 | 58.268 | - | |
26-73 | 2s22p53d 1F3-2s22p54f 3G4 | 0.30 | 59.258 | 59.43 | - | - | |
9-39 | 2s22p53p 1P1-2s22p54s 1P1 | 57.388 | 57.53 | 57.407 | - | ||
20-61 | 2s22p53d 3F3-2s22p54f 1G4 | 0.41 | 58.980 | 59.15 | 59.278 | - | |
7-39 | 2s22p53p 3D2-2s22p54s 1P1 | 56.668 | 56.79 | 56.686 | - | ||
18-37 | 2s22p53d 3P2-2p63d 1D2 | 89.874 | 87.92 | - | 89.95 | ||
10-39 | 2s22p53p 3P2-2s22p54s 1P1 | 57.874 | 58.01 | 57.893 | - | ||
27-37 | 2s22p53d 1P1-2p63d 1D2 | 106.585 | 104.77 | - | 106.66 | ||
7-31 | 2s22p53p 3D2-2p63p 3P1 | 92.793 | 90.86 | 92.832 | 92.89 | ||
18-64 | 2s22p53d 3P2-2s22p54f 3F3 | 0.27 | 58.621 | 58.76 | - | - | |
24-72 | 2s22p53d 3F2-2s22p54f 3G3 | 0.22 | 58.751 | 59.07 | 59.010 | - | |
22-67 | 2s22p53d 3D3-2s22p54f 3F4 | 0.40 | 59.590 | 59.79 | 59.607 | - | |
21-66 | 2s22p53d 1D2-2s22p54f 1F3 | 0.25 | 59.260 | 59.48 | 59.337 | - |
Notes: Lines are ordered by
decreasing intensity. The first column indicates the level indices as
given in Loch et al.
(2006).
The second column provides the transition description. The relative
intensities (photons) Int were calculated at
electron densities of 1011 and 1019 cm-3,
typical of solar flares and laboratory spectra.
are our experimental wavelengths.
are the wavelengths obtained from the scattering target energies (Loch et al. 2006),
while
are those from NIST v.3 and
are those obtained from the MR-MP calculations.
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