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Table 2:

Wavelengths and oscillator strengths of the lines analyzed.

Species
$\lambda_{\rm rest}$ (Å) $\lambda_{\rm obs}$ (Å) $\log(gf)$a $N_{\rm sat}$ (cm-2)b Comment
I  1025.722 1029.389 0.0527 ... Lyman $\beta $
I  937.803 941.080 0.0026 ... Lyman $\epsilon $
I  953.415 956.797 0.0132 $5\times10^{14}$  
I  953.655 957.031 0.0250 $3\times10^{14}$  
I  953.970 957.343 0.0350 $2\times10^{14}$  
I  963.990 967.040 0.0148 $4\times10^{14}$ Blended with P II  $\lambda963.8$
I  964.626 968.029 0.0094 $7\times10^{14}$ Barely detected
I  965.041 968.458 0.0040 $2\times10^{15}$ Not detected
I  1134.165 1138.069 0.0134 $4\times10^{14}$ Barely detected
I  1134.415 1138.303 0.0268 $2\times10^{14}$  
I  1134.980 1138.888 0.0402 $8\times10^{13}$  
I  988.773 992.209 0.0465 $1\times10^{14}$ Saturated
I  1039.230 1042.961 0.0092 $5\times10^{14}$  

Si II 
1020.699 1024.358 0.0164 $2\times10^{14}$  

II 
963.800 967.249 1.4600 $2\times10^{12}$ Blended with N I  $\lambda963.99$
II  1152.818 1156.906 0.2450 $2\times10^{13}$ Not detected

Ar I 
1048.220 1051.957 0.2630 $9\times10^{12}$  

Fe II 
1144.938 1148.976 0.1060 $3\times10^{13}$  
a Atomic data are from Morton et al. (2003), except for Fe II $\lambda$1144.938 for which we take Howk et al. (2000).
b $N_{\rm sat}$ is the maximum column density before saturation of a central component with b=2 km s-1 (Sect. 4.1.2).

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