could be measured because their lines are weaker than that of Pd and they are in regions of the lower S/N.

Lutetium
--------

We were able to detect the 3507.4Å line of in [CS 31062]{}. It has a very accurate [$gf$-value]{} and HFS constants from the study by Den Hartog [et al.]{} (1998). It is blended in CS 31062-050 with an line. This line has a [$gf$-value]{} from Moity (1983). Figure 1 shows our synthesis of the line. The hyperfine splitting of the Lu line is significant enough to noticeably broaden the line. Figure 1 shows that no amount of absorption from will account for the profile of the observed line, while the three components of the line are a good match when the S/N is taken into account.

Thorium
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A possible detection of the r-process-only element Th was one of the reasons that Cohen [et al.]{} (2003) favored an s+r scenario. Unfortunately, in CS 31062-050 the strongest Th line at $\lambda$4019Å is blended with a [$^{13}$CH]{} line (Norris, Ryan, & Beers 1997). Because we could only set large upper limits (\[Th/Fe\]$<3.0$) using the non-detection of other, non-blended Th lines in our spectra, we decided to use the line 