Table 3: Equivalent width and abundance results for the sample stars, line by line. The symbol "<'' indicates an upper limit. The stars signaled with "*'' were considered normal rather than barium stars by Smiljanic et al. (2007).

Identifiers		 El. $\lambda $ (Å) EW $\log\epsilon$(X) [X/Fe]   Identifiers El. $\lambda $ (Å) EW $\log\epsilon$(X) [X/Fe]
        (mÅ)               (mÅ)    

HD 749		   Ru I 4080.574 64 2.48 0.70   HD 106191   Hf II 4080.437 ... ... ...
HD 749   Ru I 4757.856 52 2.43 0.65   HD 106191   Hf II 4093.155 ... <1.09 <0.50
HD 749   Hf II 4080.437 56 2.27 1.45   HD 107574   Ru I 4080.574 ... ... ...
HD 749   Hf II 4093.155 107 2.27 1.45   HD 107574   Ru I 4757.856 11 3.29 2.00
HD 2454 HR 107 Ru I 4080.574 ... <2.48 <1.00   HD 107574   Hf II 4080.437 ... ... ...
HD 2454 HR 107 Ru I 4757.856 3 2.88 1.40   HD 107574   Hf II 4093.155 13 1.33 1.00
HD 2454 HR 107 Hf II 4080.437 ... <0.92 <0.40   HD 113226* HR 4932 Ru I 4080.574 31 1.86 -0.10
HD 2454 HR 107 Hf II 4093.155 ... <0.52 <0.00   HD 113226* HR 4932 Ru I 4757.856 12 1.96 0.00
HD 5424   Ru I 4080.574 71 2.19 0.90   HD 113226* HR 4932 Hf II 4080.437 9 0.80 -0.20
HD 5424   Ru I 4757.856 77 2.49 1.20   HD 113226* HR 4932 Hf II 4093.155 50 0.80 -0.20
HD 5424   Hf II 4080.437 92 2.08 1.75   HD 116713 HR 5058 Ru I 4080.574 105 2.42 0.70
HD 5424   Hf II 4093.155 ... ... ...   HD 116713 HR 5058 Ru I 4757.856 77 2.62 0.90
HD 8270 HR 391 Ru I 4080.574 8 2.37 0.95   HD 116713 HR 5058 Hf II 4080.437 75 1.76 1.00
HD 8270 HR 391 Ru I 4757.856 6 2.42 1.00   HD 116713 HR 5058 Hf II 4093.155 117 1.76 1.00
HD 8270 HR 391 Hf II 4080.437 9 1.16 0.70   HD 116869   Ru I 4080.574 59 2.02 0.50
HD 8270 HR 391 Hf II 4093.155 11 1.36 0.90   HD 116869   Ru I 4757.856 46 2.22 0.70
HD 9362* HR 440 Ru I 4080.574 25 1.55 0.05   HD 116869   Hf II 4080.437 68 1.51 0.95
HD 9362* HR 440 Ru I 4757.856 15 1.75 0.25   HD 116869   Hf II 4093.155 63 1.26 0.70
HD 9362* HR 440 Hf II 4080.437 16 0.69 0.15   HD 123396   Ru I 4080.574 58 1.45 0.80
HD 9362* HR 440 Hf II 4093.155 35 0.54 0.00   HD 123396   Ru I 4757.856 48 1.65 1.00
HD 12392   Ru I 4080.574 76 3.22 1.50   HD 123396   Hf II 4080.437 72 1.39 1.70
HD 12392   Ru I 4757.856 61 3.02 1.30   HD 123396   Hf II 4093.155 87 1.59 1.90
HD 12392   Hf II 4080.437 63 2.42 1.66   HD 139195 HR 5802 Ru I 4080.574 39 2.07 0.25
HD 12392   Hf II 4093.155 95 2.42 1.66   HD 139195 HR 5802 Ru I 4757.856 20 2.07 0.25
HD 13551   Ru I 4080.574 8 2.40 1.00   HD 139195 HR 5802 Hf II 4080.437 22 1.06 0.20
HD 13551   Ru I 4757.856 8 2.70 1.30   HD 139195 HR 5802 Hf II 4093.155 49 1.16 0.30
HD 13551   Hf II 4080.437 21 1.39 0.95   HD 147609   Ru I 4080.574 ... <2.69 <1.30
HD 13551   Hf II 4093.155 23 1.54 1.10   HD 147609   Ru I 4757.856 15 3.09 1.70
HD 13611* HR 649 Ru I 4080.574 23 1.95 0.25   HD 147609   Hf II 4080.437 ... <2.03 <1.60
HD 13611* HR 649 Ru I 4757.856 19 2.25 0.55   HD 147609   Hf II 4093.155 ... ... ...
HD 13611* HR 649 Hf II 4080.437 33 0.99 0.25   HD 150862   Ru I 4080.574 ... ... ...
HD 13611* HR 649 Hf II 4093.155 67 0.94 0.20   HD 150862   Ru I 4757.856 1 2.99 1.25
HD 20894* HR 1016 Ru I 4080.574 17 1.88 0.15   HD 150862   Hf II 4080.437 ... ... ...
HD 20894* HR 1016 Ru I 4757.856 13 2.08 0.35   HD 150862   Hf II 4093.155 12 1.48 0.70
HD 20894* HR 1016 Hf II 4080.437 18 0.92 0.15   HD 181053 HR 5802 Ru I 4080.574 47 1.80 0.15
HD 20894* HR 1016 Hf II 4093.155 68 1.28 0.51   HD 181053 HR 5802 Ru I 4757.856 27 1.90 0.25
HD 22589   Ru I 4080.574 12 2.12 0.55   HD 181053 HR 5802 Hf II 4080.437 30 0.94 0.25
HD 22589   Ru I 4757.856 5 2.27 0.70   HD 181053 HR 5802 Hf II 4093.155 71 0.99 0.30
HD 22589   Hf II 4080.437 18 1.06 0.45   HD 188985   Ru I 4080.574 ... ... ...
HD 22589   Hf II 4093.155 49 1.31 0.70   HD 188985   Ru I 4757.856 13 3.09 1.55
HD 26967* HR 1326 Ru I 4080.574 145 1.84 0.00   HD 188985   Hf II 4080.437 ... ... ...
HD 26967* HR 1326 Ru I 4757.856 87 1.84 0.00   HD 188985   Hf II 4093.155 34 1.68 1.10
HD 26967* HR 1326 Hf II 4080.437 92 0.78 -0.10   HD 202109 HR 8115 Ru I 4080.574 42 1.90 0.10
HD 26967* HR 1326 Hf II 4093.155 90 0.78 -0.10   HD 202109 HR 8115 Ru I 4757.856 26 2.05 0.25
HD 27271   Ru I 4080.574 58 2.20 0.45   HD 202109 HR 8115 Hf II 4080.437 27 0.99 0.15
HD 27271   Ru I 4757.856 29 2.05 0.30   HD 202109 HR 8115 Hf II 4093.155 93 1.09 0.25
HD 27271   Hf II 4080.437 73 1.49 0.70   HD 204075 HR 8204 Ru I 4080.574 ... ... ...
HD 27271   Hf II 4093.155 67 1.49 0.70   HD 204075 HR 8204 Ru I 4757.856 60 3.50 1.75
HD 46407 HR 2392 Ru I 4080.574 87 2.70 0.95   HD 204075 HR 8204 Hf II 4080.437 ... ... ...
HD 46407 HR 2392 Ru I 4757.856 74 2.90 1.15   HD 204075 HR 8204 Hf II 4093.155 118 1.79 1.00
HD 46407 HR 2392 Hf II 4080.437 86 1.94 1.15   HD 205011   Ru I 4080.574 66 2.05 0.35
HD 46407 HR 2392 Hf II 4093.155 92 1.94 1.15   HD 205011   Ru I 4757.856 40 2.15 0.45
HD 48565   Ru I 4080.574 12 2.52 1.30   HD 205011   Hf II 4080.437 46 1.29 0.55
HD 48565   Ru I 4757.856 15 2.97 1.75   HD 205011   Hf II 4093.155 92 1.34 0.60
HD 48565   Hf II 4080.437 34 1.66 1.40   HD 210709   Ru I 4080.574 67 2.00 0.20
HD 48565   Hf II 4093.155 25 1.66 1.40   HD 210709   Ru I 4757.856 40 2.30 0.50
HD 76225   Ru I 4080.574 3 2.83 1.30   HD 210709   Hf II 4080.437 36 1.34 0.50
HD 76225   Ru I 4757.856 10 3.23 1.70   HD 210709   Hf II 4093.155 64 1.04 0.20
HD 76225   Hf II 4080.437 33 1.67 1.10   HD 210910   Ru I 4080.574 ... <1.47 <0.00
HD 76225   Hf II 4093.155 20 1.47 0.90   HD 210910   Ru I 4757.856 ... 1.47 0.00
HD 87080   Ru I 4080.574 28 2.80 1.40   HD 210910   Hf II 4080.437 ... <0.81 <0.30
HD 87080   Ru I 4757.856 29 3.00 1.60   HD 210910   Hf II 4093.155 ... <0.51 <0.00
HD 87080   Hf II 4080.437 51 2.24 1.80   HD 220009* HR 8878 Ru I 4080.574 53 1.27 0.10
HD 87080   Hf II 4093.155 34 2.04 1.60   HD 220009* HR 8878 Ru I 4757.856 27 1.22 0.05
HD 89948   Ru I 4080.574 5 2.54 1.00   HD 220009* HR 8878 Hf II 4080.437 21 0.21 0.00
HD 89948   Ru I 4757.856 8 2.79 1.25   HD 220009* HR 8878 Hf II 4093.155 50 0.21 0.00
HD 89948   Hf II 4080.437 17 1.48 0.90   HD 222349   Ru I 4080.574 16 2.71 1.50
HD 89948   Hf II 4093.155 19 1.38 0.80   HD 222349   Ru I 4757.856 5 3.01 1.80
HD 92545   Ru I 4080.574 ... ... ...   HD 222349   Hf II 4080.437 17 1.55 1.30
HD 92545   Ru I 4757.856 5 3.02 1.30   HD 222349   Hf II 4093.155 21 1.55 1.30
HD 92545   Hf II 4080.437 ... ... ...   BD+18 5215   Ru I 4080.574 3 2.81 1.50
HD 92545   Hf II 4093.155 11 1.26 0.50   BD+18 5215   Ru I 4757.856 ... ... ...
HD 104979 HR 4608 Ru I 4080.574 47 2.04 0.55   BD+18 5215   Hf II 4080.437 20 1.55 1.20
HD 104979 HR 4608 Ru I 4757.856 33 2.24 0.75   BD+18 5215   Hf II 4093.155 15 1.55 1.20
HD 104979 HR 4608 Hf II 4080.437 54 1.18 0.65   HD 223938   Ru I 4080.574 38 1.99 0.50
HD 104979 HR 4608 Hf II 4093.155 77 1.08 0.55   HD 223938   Ru I 4757.856 23 2.24 0.75
HD 106191   Ru I 4080.574 ... ... ...   HD 223938   Hf II 4080.437 36 1.58 1.05
HD 106191   Ru I 4757.856 8 3.25 1.70   HD 223938   Hf II 4093.155 58 1.58 1.05
$\log\epsilon$(X) = ( $\log{n_{\rm X}/n_{\rm H}}$) + 12 and [X/Fe] =  $\log\epsilon {\rm (X)}_\ast-\log\epsilon ({\rm X})_\odot\rm -[Fe/H]$.

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