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Home All issues Volume 508 / No 1 (December II 2009) A&A, 508 1 (2009) 513-524 Full HTML
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Table 3:

List of strongest Fe VIII lines in the 100-500 Å range.

i-j 		Levels Int gf G00 Z03 D Aji(s-1) $\lambda_{\rm exp}$(Å) $\lambda_{\rm th}$(Å) ID
2-49 3p63d 2D5/2-3p53d2 2D5/2 1.0 7.06 9.1 7.2 $2.8 \times 10^{11}$ 168.173 159.73 G65
2-46 3p63d 2D5/2-3p53d2 2F7/2 0.90 3.92 5.8 4.2 $9.5 \times 10^{10}$ 185.213 178.09 G65
1-50 3p63d 2D3/2-3p53d2 2D3/2 0.58 4.56 5.9 4.6 $2.7 \times 10^{11}$ 167.486 159.20 G65
2-48 3p63d 2D5/2-3p53d2 2P3/2 0.57 3.82 4.3 3.7 $2.2 \times 10^{11}$ 168.544 162.16 RR80
1-45 3p63d 2D3/2-3p53d2 2F5/2 0.58 2.80 4.1 2.9 $9.0 \times 10^{10}$ 186.599 179.25 G65
1-47 3p63d 2D3/2-3p53d2 2P1/2 0.29 2.10 2.4 2.0 $2.4 \times 10^{11}$ 168.929 162.43 RR80
2-43 3p63d 2D5/2-3p64p 2P3/2 0.29 0.67 0.60 - $3.0 \times 10^{10}$ 194.661 191.39 RR80
2-54 3p63d 2D5/2-3p64f 2F7/2 0.14 4.30 4.0 - $2.1 \times 10^{11}$ 131.240 129.02 KW37
1-42 3p63d 2D3/2-3p64p 2P1/2 0.17 0.38 0.38 - $3.3 \times 10^{10}$ 195.972 192.88 ? RR80
1-53 3p63d 2D3/2-3p64f 2F5/2 $9.0\times 10^{-2}$ 2.97 2.8 - $1.9 \times 10^{11}$ 130.941 128.71 KW37
2-26 3p63d 2D5/2-3p53d2 2F7/2 0.14 0.14 0.10 - $2.2 \times 10^{9}$ 224.305 223.88 RR80
2-6 3p63d 2D5/2-3p53d2 4D7/2 0.15 $2.1\times 10^{-4}$ $2.2 \times 10^{-4}$ - $2.8 \times 10^{6}$ 253.956 257.79 N
2-22 3p63d 2D5/2-3p53d2 2F7/2 0.12 $5.6\times 10^{-2}$ $5.2 \times 10^{-2}$ - $8.8 \times 10^{8}$ 231.097 231.15 RR80
2-9 3p63d 2D5/2-3p53d2 4G7/2 $9.9 \times 10^{-2}$ $1.0 \times 10^{-4}$ $7.0 \times 10^{-5}$ - $1.4\times 10^{6}$ - 243.92  
2-17 3p63d 2D5/2-3p53d2 4F7/2 $9.5 \times 10^{-2}$ $8.1 \times 10^{-4}$ $4.8 \times 10^{-4}$ - $1.2 \times 10^{7}$ - 235.41  
2-21 3p63d 2D5/2-3p64s 2S1/2 $8.9 \times 10^{-2}$ - 0.0 - $6.5 \times 10^{5}$ - 231.69  
1-30 3p63d 2D3/2-3p53d2 2F5/2 $8.1\times 10^{-2}$ 0.12 0.10 - $2.9\times 10^{9}$ 217.691 217.17 RR80
1-49 3p63d 2D3/2-3p53d2 2D5/2 $6.1 \times 10^{-2}$ 0.43 0.57 0.51 $1.7\times 10^{10}$ 167.655 159.24 G65
2-50 3p63d 2D5/2-3p53d2 2D3/2 $5.6\times 10^{-2}$ 0.44 0.64 0.51 $2.6 \times 10^{10}$ 168.003 159.69 G65
1-48 3p63d 2D3/2-3p53d2 2P3/2 $5.5 \times 10^{-2}$ 0.37 0.48 0.41 $2.2 \times 10^{10}$ 168.024 161.65 RR80
2-5 3p63d 2D5/2-3p53d2 4D5/2 $8.3 \times 10^{-2}$ $2.4 \times 10^{-4}$ $2.2 \times 10^{-4}$ - $4.0\times 10^{6}$ 255.350 259.31 N
2-24 3p63d 2D5/2-3p53d2 2P3/2 $7.3 \times 10^{-2}$ $2.2 \times 10^{-2}$ $1.6\times 10^{-2}$ $2.1 \times 10^{-2}$ $7.2 \times 10^{8}$ 225.396 225.29 N
2-31 3p63d 2D5/2-3p53d2 4D7/2 $7.0 \times 10^{-2}$ $1.3\times 10^{-4}$ $1.1 \times 10^{-4}$ - $2.2 \times 10^{6}$ - 217.51  
2-16 3p63d 2D5/2-3p53d2 4F9/2 $7.2\times 10^{-2}$ $4.5 \times 10^{-12}$ 0.0 - 45. - 235.87  
1-19 3p63d 2D3/2-3p53d2 2F5/2 $6.7\times 10^{-2}$ $4.1\times 10^{-2}$ $3.2 \times 10^{-2}$ - $8.5 \times 10^{8}$ 231.884 232.05 RR80
2-18 3p63d 2D5/2-3p53d2 2D5/2 $6.7\times 10^{-2}$ $8.8\times 10^{-4}$ $1.6 \times 10^{-6}$ - $1.8\times 10^{7}$ - 233.49  
2-27 3p63d 2D5/2-3p53d2 2G7/2 $6.3 \times 10^{-2}$ $1.1 \times 10^{-2}$ $3.6 \times 10^{-2}$ - $1.8\times 10^{8}$ 222.190 222.57 N
2-41 3p63d 2D5/2-3p53d2 2P3/2 $5.2 \times 10^{-2}$ $9.9 \times 10^{-2}$ 0.19 0.13 $4.3 \times 10^{9}$ 197.362 194.03 RR80
1-21 3p63d 2D3/2-3p64s 2S1/2 $5.9 \times 10^{-2}$ - 0.0 - $4.3 \times 10^{5}$ - 230.66  
1-36 3p63d 2D3/2-3p53d2 2D5/2 $5.3 \times 10^{-2}$ $3.7 \times 10^{-3}$ $2.2 \times 10^{-3}$ - $9.5\times 10^{7}$ 207.124 205.01 N
2-10 3p63d 2D5/2-3p53d2 4P5/2 $5.9 \times 10^{-2}$ $1.3\times 10^{-4}$ $1.0 \times 10^{-4}$ - $2.5\times 10^{6}$ - 243.30  
1-4 3p63d 2D3/2-3p53d2 4D3/2 $5.1\times 10^{-2}$ $1.1 \times 10^{-4}$ $1.1 \times 10^{-4}$ - $2.8 \times 10^{6}$ 255.110 259.05 N
2-20 3p63d 2D5/2-3p53d2 2D3/2 $4.5 \times 10^{-2}$ $6.0\times 10^{-3}$ $3.3\times 10^{-3}$ - $1.9\times 10^{8}$ - 232.52  
2-40 3p63d 2D5/2-3p53d2 2G7/2 $3.9 \times 10^{-2}$ $2.2 \times 10^{-2}$ $1.8\times 10^{-2}$ - $4.3\times 10^{8}$ 204.704 203.12 N
1-15 3p63d 2D3/2-3p53d2 4F5/2 $4.2\times 10^{-2}$ $5.8\times 10^{-3}$ $3.9\times 10^{-3}$ - $1.2\times 10^{8}$ - 235.12  
2-32 3p63d 2D5/2-3p53d2 4D5/2 $3.5\times 10^{-2}$ $2.8 \times10^{-3}$ $1.6\times 10^{-3}$ - $6.5\times 10^{7}$ - 216.87  
1-14 3p63d 2D3/2-3p53d2 4F3/2 $3.8\times 10^{-2}$ $5.7\times 10^{-3}$ $4.9 \times 10^{-3}$ - $1.7 \times 10^{8}$ - 235.83  
1-43 3p63d 2D3/2-3p64p 2P3/2 $3.1 \times 10^{-2}$ $7.1\times 10^{-2}$ $6.1 \times 10^{-2}$ - $3.2 \times 10^{9}$ 193.968 190.69 RR80
1-23 3p63d 2D3/2-3p53d2 2P1/2 $3.4\times 10^{-2}$ $1.5\times 10^{-2}$ $1.0 \times 10^{-2}$ - $9.4\times 10^{8}$ 227.290 227.10 N
2-45 3p63d 2D5/2-3p53d2 2F5/2 $2.5 \times 10^{-2}$ 0.12 0.21 0.20 $3.9\times 10^{9}$ 187.240 179.87 RR80
1-35 3p63d 2D3/2-3p53d2 2D3/2 $2.2 \times 10^{-2}$ $2.6\times 10^{-3}$ $1.9\times 10^{-3}$ - $9.8\times 10^{7}$ - 206.68  
2-11 3p63d 2D5/2-3p53d2 4G5/2 $2.4\times 10^{-2}$ $5.5\times 10^{-5}$ $6.2\times 10^{-5}$ - $1.1\times 10^{6}$ - 242.64  
1-3 3p63d 2D3/2-3p53d2 4D1/2 $2.5 \times 10^{-2}$ $1.6\times 10^{-5}$ $1.8\times 10^{-5}$ - $8.0\times 10^{5}$ 255.684 259.66 N
1-44 3p63d 2D3/2-3p53d2 2P1/2 $1.6\times 10^{-2}$ $4.0\times 10^{-2}$ $5.9 \times 10^{-2}$ $6.0\times 10^{-2}$ $3.6\times 10^{9}$ 192.004 188.74 ? RR80
2-12 3p63d 2D5/2-3p53d2 4P3/2 $1.9\times 10^{-2}$ $7.6\times 10^{-5}$ $1.2\times 10^{-4}$ - $2.2 \times 10^{6}$ - 241.53  
2-25 3p63d 2D5/2-3p53d2 2H11/2 1.6 10-2 $1.0\times 10^{-10}$ 0.0 - 1.1 - 224.95  
2-33 3p63d 2D5/2-3p53d2 4D3/2 $1.6\times 10^{-2}$ $2.9\times 10^{-3}$ $2.3 \times 10^{-3}$ - $1.0 \times 10^{8}$ - 215.96  
2-15 3p63d 2D5/2-3p53d2 4F5/2 $1.6\times 10^{-2}$ $2.3 \times 10^{-3}$ $2.6\times 10^{-3}$ - $4.6\times 10^{7}$ - 236.19  
2-28 3p63d 2D5/2-3p53d2 2G9/2 $1.5\times 10^{-2}$ $8.2 \times 10^{-11}$ 0.0 - 9.7 - 221.16  
2-37 3p63d 2D5/2-3p53d2 4S3/2 $1.3 \times 10^{-2}$ $7.9 \times 10^{-3}$ $6.2 \times 10^{-3}$ - $3.1\times 10^{8}$ 207.124 204.74  
2-30 3p63d 2D5/2-3p53d2 2F5/2 $1.3 \times 10^{-2}$ $2.0 \times 10^{-2}$ $1.8\times 10^{-2}$ - $4.7\times 10^{8}$ 218.564 218.09 RR80
1-10 3p63d 2D3/2-3p53d2 4P5/2 $1.4 \times 10^{-2}$ $3.1 \times 10^{-5}$ $2.7\times 10^{-5}$ - $6.0 \times 10^{5}$ - 242.16  
1-13 3p63d 2D3/2-3p53d2 4P1/2 $1.4 \times 10^{-2}$ $1.5 \times 10^{-5}$ $2.5 \times 10^{-5}$ - $8.7 \times 10^{5}$ - 239.13  
2-53 3p63d 2D5/2-3p64f 2F5/2 $6.5\times 10^{-3}$ 0.22 0.20 - $1.4 \times 10^{10}$ 131.257 129.03 RR80
1-12 3p63d 2D3/2-3p53d2 4P3/2 $1.2\times 10^{-2}$ $4.8 \times 10^{-5}$ $5.1\times 10^{-5}$ - $1.4\times 10^{6}$ - 240.40  
1-41 3p63d 2D3/2-3p53d2 2P3/2 $9.6 \times 10^{-3}$ $1.8\times 10^{-2}$ $2.8\times 10^{-2}$ $1.5\times 10^{-2}$ $7.8\times 10^{8}$ 196.650 193.30 RR80
2-35 3p63d 2D5/2-3p53d2 2D3/2 $8.7 \times 10^{-3}$ $1.0 \times 10^{-3}$ $6.8\times 10^{-4}$ - $4.0 \times 10^{7}$ - 207.51  
1-34 3p63d 2D3/2-3p53d2 4D1/2 $8.9 \times 10^{-3}$ $2.7 \times 10^{-3}$ $2.0\times 10^{-3}$ - $1.9\times 10^{8}$ - 214.21  
2-8 3p63d 2D5/2-3p53d2 4G9/2 $9.6 \times 10^{-3}$ $1.1 \times 10^{-12}$ 0.0 - 0.82 - 245.12  
2-19 3p63d 2D5/2-3p53d2 2F5/2 $8.9 \times 10^{-3}$ $5.5 \times 10^{-3}$ $6.0\times 10^{-3}$ - $1.1\times 10^{8}$ 232.876 233.10 RR80

Notes: the relative intensities (photons) ${\rm Int}=N_{j} A_{ji}/N_{\rm e}$ are normalised to the strongest transition and were calculated at an electron density of 109 cm-3and log T[K] = 5.6. Weighted oscillator strengths gf and A-values (s-1) are from the benchmark calculation. The gf values from G00 and the Z03 (case D) calculation are also listed. $\lambda_{\rm exp}$ are our experimental wavelengths, while $\lambda_{\rm th}$ are the theoretical ones from the G00 energies. The last column (ID) provides a key to previous identifications. N indicates a new one proposed here.

Source LaTeX | All tables | In the text

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