Free Access
[Å]
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Ion. stage |
[eV]
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[108 1/s]
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[Å]
|
Ion. stage |
![$\chi_{\rm low} [eV]$](/articles/aa/full_html/2009/47/aa12660-09/img161.png){kind=small}
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[108 1/s]
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| 4993.35 | 2 | 2.80 | -3.73 | -31.60 | 3.0500 | 6252.57 | 1 | 2.40 | -1.56 | -31.92 | 0.87000 |
| 4994.14 | 1 | 0.91 | -3.01 | -31.97 | 0.15000 | 6297.80 | 1 | 2.22 | -2.71 | -31.86 | 1.5500 |
| 5127.37 | 1 | 0.91 | -3.20 | -31.97 | 0.16600 | 6301.51 | 1 | 3.65 | -0.67 | -30.70 | 0.80500 |
| 5197.58 | 2 | 3.23 | -2.31 | -31.80 | 3.0300 | 6330.85 | 1 | 4.73 | -1.15 | -31.69 | 2.3840 |
| 5198.72 | 1 | 2.22 | -2.12 | -31.50 | 1.6100 | 6335.34 | 1 | 2.20 | -2.22 | -31.86 | 1.6600 |
| 5217.40 | 1 | 3.21 | -1.08 | -30.60 | 0.76000 | 6336.83 | 1 | 3.69 | -0.80 | -30.70 | 0.81100 |
| 5223.19 | 1 | 3.64 | -2.25 | -31.91 | 0.78600 | 6369.46 | 2 | 2.89 | -4.19 | -31.50 | 2.9000 |
| 5234.63 | 2 | 3.22 | -2.23 | -31.80 | 3.0700 | 6380.75 | 1 | 4.19 | -1.24 | -31.70 | 0.73503 |
| 5242.50 | 1 | 3.63 | -0.87 | -31.70 | 0.57500 | 6393.61 | 1 | 2.43 | -1.39 | -31.92 | 0.93200 |
| 5264.81 | 2 | 3.23 | -3.11 | -32.19 | 4.1100 | 6411.66 | 1 | 3.65 | -0.56 | -30.70 | 0.80300 |
| 5281.80 | 1 | 3.04 | -0.91 | -30.90 | 1.0200 | 6416.93 | 2 | 3.89 | -2.67 | -31.90 | 3.3700 |
| 5284.11 | 2 | 2.89 | -3.12 | -32.11 | 3.4300 | 6430.85 | 1 | 2.18 | -2.02 | -31.86 | 1.6500 |
| 5295.32 | 1 | 4.42 | -1.52 | -31.15 | 1.8380 | 6432.68 | 2 | 2.89 | -3.63 | -31.50 | 2.9000 |
| 5302.31 | 1 | 3.28 | -0.75 | -30.60 | 0.74900 | 6436.41 | 1 | 4.19 | -2.39 | -31.96 | 0.30403 |
| 5325.56 | 2 | 3.22 | -3.22 | -31.80 | 3.1000 | 6456.39 | 2 | 3.90 | -2.09 | -31.90 | 3.3700 |
| 5339.94 | 1 | 3.27 | -0.65 | -30.60 | 0.74900 | 6481.88 | 1 | 2.28 | -2.90 | -31.91 | 1.5500 |
| 5364.88 | 1 | 4.45 | 0.39 | -31.15 | 1.8550 | 6498.94 | 1 | 0.96 | -4.62 | -32.02 | 0.000435 |
| 5367.48 | 1 | 4.42 | 0.49 | -31.15 | 1.8500 | 6516.09 | 2 | 2.89 | -3.34 | -31.50 | 2.9100 |
| 5379.58 | 1 | 3.69 | -1.44 | -31.70 | 0.57500 | 6591.32 | 1 | 4.59 | -2.01 | -31.80 | 1.4000 |
| 5393.17 | 1 | 3.24 | -0.74 | -30.60 | 0.74800 | 6593.88 | 1 | 2.43 | -2.29 | -31.92 | 0.86200 |
| 5414.07 | 2 | 3.22 | -3.61 | -32.19 | 4.1200 | 6608.03 | 1 | 2.28 | -3.99 | -31.91 | 1.6600 |
| 5425.25 | 2 | 3.20 | -3.28 | -31.80 | 2.9900 | 6627.55 | 1 | 4.55 | -1.48 | -31.44 | 1.7530 |
| 5497.52 | 1 | 1.01 | -2.82 | -31.99 | 0.14200 | 6704.48 | 1 | 4.22 | -2.62 | -31.16 | - |
| 5522.45 | 1 | 4.21 | -1.40 | -30.80 | 0.89800 | 6710.32 | 1 | 1.48 | -4.84 | -31.97 | 0.16600 |
| 5534.85 | 2 | 3.24 | -2.83 | -32.18 | 2.9900 | 6713.75 | 1 | 4.80 | -1.42 | -31.30 | 2.3550 |
| 5546.51 | 1 | 4.37 | -1.05 | -31.20 | 1.7860 | 6725.36 | 1 | 4.10 | -2.21 | -31.37 | 2.0910 |
| 5560.22 | 1 | 4.43 | -0.96 | -31.50 | 1.6410 | 6733.15 | 1 | 4.64 | -1.43 | -31.37 | 2.2680 |
| 5576.10 | 1 | 3.43 | -0.79 | -30.85 | 0.75300 | 6750.16 | 1 | 2.42 | -2.53 | -31.95 | 0.0770 |
| 5611.36 | 1 | 3.64 | -2.93 | -31.91 | 1.2500 | 6786.87 | 1 | 4.19 | -1.90 | -31.36 | 1.9860 |
| 5618.64 | 1 | 4.21 | -1.22 | -31.46 | 1.0450 | 6806.85 | 1 | 2.73 | -3.11 | -31.83 | 1.0200 |
| 5636.70 | 1 | 3.64 | -2.52 | -31.94 | 0.39000 | 6810.27 | 1 | 4.61 | -0.94 | -30.90 | 2.3010 |
| 5638.27 | 1 | 4.22 | -0.65 | -31.00 | 1.9430 | 6820.37 | 1 | 4.64 | -1.11 | -30.90 | 2.2200 |
| 5651.47 | 1 | 4.47 | -1.77 | -31.30 | 1.6310 | 6837.01 | 1 | 4.59 | -1.74 | -31.81 | 0.52405 |
| 5679.03 | 1 | 4.65 | -0.64 | -30.80 | 1.3990 | 6843.66 | 1 | 4.55 | -0.73 | -31.10 | 1.9230 |
| 5741.85 | 1 | 4.26 | -1.63 | -31.10 | 2.1080 | 6857.25 | 1 | 4.08 | -2.08 | -31.40 | 0.25303 |
| 5855.08 | 1 | 4.61 | -1.54 | -31.75 | 1.9110 | 6862.50 | 1 | 4.56 | -1.43 | -31.30 | 3.5400 |
| 5856.09 | 1 | 4.29 | -1.55 | -31.91 | 0.86200 | 6936.50 | 1 | 4.61 | -2.20 | -31.69 | 3.2000 |
| 5862.36 | 1 | 4.55 | -0.16 | -31.30 | 1.8970 | 6945.21 | 1 | 2.42 | -2.39 | -31.95 | 0.15700 |
| 5930.19 | 1 | 4.65 | -0.02 | -31.30 | 1.8530 | 6978.86 | 1 | 2.48 | -2.39 | -31.95 | 0.07700 |
| 5956.70 | 1 | 0.86 | -4.54 | -32.01 | 0.000271 | 7219.69 | 1 | 4.08 | -1.49 | -31.91 | 1.6300 |
| 5991.38 | 2 | 3.15 | -3.59 | -31.60 | 3.4600 | 7222.40 | 2 | 3.89 | -3.26 | -31.60 | 4.1400 |
| 6027.06 | 1 | 4.08 | -1.02 | -31.91 | 0.88503 | 7224.48 | 2 | 3.89 | -3.24 | -31.60 | 4.1400 |
| 6056.01 | 1 | 4.73 | -0.31 | -30.80 | 1.8480 | 7301.57 | 2 | 3.89 | -3.69 | -32.18 | 3.0700 |
| 6065.49 | 1 | 2.61 | -1.38 | -31.92 | 1.0200 | 7306.57 | 1 | 4.18 | -1.54 | -30.80 | 1.6710 |
| 6084.11 | 2 | 3.20 | -3.84 | -31.60 | 3.4300 | 7401.69 | 1 | 4.19 | -1.52 | -31.90 | 0.70303 |
| 6093.65 | 1 | 4.61 | -1.32 | -31.75 | 1.9350 | 7411.16 | 1 | 4.28 | -0.32 | -30.80 | 1.7020 |
| 6096.67 | 1 | 3.98 | -1.79 | -31.10 | 0.45250 | 7421.56 | 1 | 4.64 | -1.70 | -31.82 | 2.5010 |
| 6113.32 | 2 | 3.22 | -4.16 | -31.60 | 3.4100 | 7445.76 | 1 | 4.26 | -0.10 | -30.80 | 1.6990 |
| 6149.25 | 2 | 3.89 | -2.75 | -31.90 | 3.3900 | 7454.00 | 1 | 4.19 | -2.34 | -31.90 | 1.4500 |
| 6151.62 | 1 | 2.18 | -3.29 | -31.86 | 1.5500 | 7479.70 | 2 | 3.89 | -3.70 | -32.18 | 3.1000 |
| 6157.73 | 1 | 4.08 | -1.10 | -31.70 | 0.50203 | 7491.66 | 1 | 4.30 | -0.95 | -30.80 | 1.6920 |
| 6173.34 | 1 | 2.22 | -2.84 | -31.86 | 1.6700 | 7495.08 | 1 | 4.22 | 0.04 | -30.80 | 1.6810 |
| 6200.32 | 1 | 2.61 | -2.31 | -31.92 | 1.0300 | 7498.53 | 1 | 4.14 | -2.16 | -31.90 | 1.1600 |
| 6213.44 | 1 | 2.22 | -2.51 | -31.86 | 1.6500 | 7515.84 | 2 | 3.90 | -3.45 | -31.60 | 4.0900 |
| 6226.74 | 1 | 3.88 | -2.11 | -31.10 | 0.54140 | 7540.44 | 1 | 2.72 | -3.81 | -31.85 | 0.93200 |
| 6232.65 | 1 | 3.65 | -1.20 | -30.70 | 0.80600 | 7568.91 | 1 | 4.28 | -0.82 | -30.80 | 1.6990 |
| 6239.94 | 2 | 3.89 | -3.50 | -31.90 | 3.3800 | 7583.80 | 1 | 3.02 | -1.80 | -31.80 | 1.0200 |
| 6240.65 | 1 | 2.22 | -3.27 | -31.95 | 0.15700 | 7711.73 | 2 | 3.90 | -2.56 | -31.60 | 4.1200 |
| 6246.33 | 1 | 3.60 | -0.73 | -30.70 | 0.79600 | 7748.28 | 1 | 2.95 | -1.56 | -31.80 | 1.0200 |
| 6247.56 | 2 | 3.89 | -2.34 | -31.90 | 3.3800 | 7844.56 | 1 | 4.83 | -1.73 | -31.59 | 2.3380 |
(1) Central wavelength, (2) ionization stage, (3) lower excitation
potential, (4) oscillator strength, (5) van der Waals damping constant,
(6) radiative damping constant. The effect of quadratic Stark
broadening (
)
on weak iron lines is negligible so that in this work, it is not taken
into account for these lines. The radiation damping constant (
)
is calculated with the classical formula in case it is missing in the table.
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