\begin{table}%T6 %\centering \par \caption{Abundance ratios derived and atomic parameters adopted.} \label{t6} \begin{tabular}{llllrrrrrrrr} \hline\hline Species & $\lambda$ & $\chi_{\rm ex}$ & $C_6$ & \multicolumn{2}{c}{log~$gf$} & \multicolumn{3}{c}{[X/Fe]} & \multicolumn{2}{c}{{\it EW} (m${\rm \AA}$)} \\ \cline{5-6} \cline{7-9} \\ & (${\rm \AA}$) & (eV) & & ZOC04 & present & Arcturus & HP1-2 & HP1-3 & \multicolumn{2}{c}{HP1-2} & HP1-3 \\ \hline [OI] & 6300.311 & 0.00 &0.30E-31 & --9.716 &--9.716 &+0.20 & +0.4 & +0.4 & 34.8 & 33.2 \\ %ScII & 6300.67 & 1.50 & & hfs & ... & & & \\ NaI & 6154.230 & 2.10 & 0.90E-31 & --1.56$^1$ & --1.56 & --0.2 & 0.0 & +0.0 & 19.0 & 33.8 & \\ NaI & 6160.753 & 2.10 & 0.30E-31 & --1.26$^1$ & --1.26 & --0.2 & 0.0 & +0.0: & 22.0 & -- & \\ % MgI & 6318.720 & 5.11 & 0.30E-31 & --2.10$^2$ & --2.10 & +0.30 & 0.0 & +0.20 &16.2 & 32.4 & \\ MgI & 6319.242 & 5.11 & 0.30E-31 & --2.36$^2$ & --2.36 & +0.30 & 0.0 &+0.20 &12.8 &22.6 & \\ MgI & 6319.490 & 5.11 & 0.30E-31 & --2.80$^2$ & --2.90 & +0.30 & -- & +0.20 & -- & 3.6 & \\ MgI & 6765.450 & 5.75 & 0.30E-31 & --1.94$^3$ & --1.94 & +0.30 & 0.0 & +0.20: & 7.4 & 7.1 & \\ % SiI & 5948.548 & 5.08 & 2.19E-30$^{a}$ & --1.17$^2$ & --1.17 & +0.25 & +0.3 &+0.3 & 80.8 & 58.2 & \\ SiI & 6142.494 & 5.62 & 0.30E-31 & --1.50$^2$ & --1.58 & +0.25 & +0.3 &+0.3 & 22.3 & 18.7 & \\ SiI & 6145.020 & 5.61 & 0.30E-31 & --1.45$^2$ & --1.5 & +0.25 & +0.3 & +0.3 & 21.0 & 20.0 & \\ SiI & 6155.142 & 5.62 & 0.30E-30 & --0.85$^2$ & --0.85 & +0.35 & +0.3 & +0.3 & 53.1 & 55.4 & \\ SiI & 6237.328 & 5.61 & 0.30E-30 & --1.01$^3$ & --1.1 & +0.25 & +0.2 &+0.3 & 29.6 & 39.0 & \\ SiI & 6243.823 & 5.61 & 0.30E-32 & --1.30$^4$ & --1.30 & +0.25 & -- & +0.2 & -- & 19.7 & \\ SiI & 6414.987 & 5.87 & 0.30E-30 & --1.13$^2$ & --1.13 & +0.35 & -- &+0.3 & -- & 21.7 & \\ SiI & 6721.844 & 5.86 & 0.90E-30 & --1.17$^3$ & --1.17 & +0.25 & +0.3 & +0.3 & 23.5 & 30.5 & \\ % CaI & 6102.727 & 1.88 & 4.54E-31$^{a}$ & --0.79$^1$ & --0.93 & +0.25 & +0.1 & +0.1 & 137.7 & 143.8 & \\ CaI & 6156.030 & 2.52 & 4.0E-31$^{aa}$ & --2.39$^2$ & --2.59 & +0.20 & --0.1 & +0.2 & 2.3 & 14.5 & \\ CaI & 6161.295 & 2.51 & 4.0E-31$^{aa}$ & --1.02$^1$ & --1.42 & +0.10 & +0.0 & +0.1 & 37.2 & -- & \\ CaI & 6162.167 & 1.89 & 3.0E-31$^{aa}$ & --0.09$^1$ & --0.09 & --0.10 & +0.0 & +0.1 & 200.0 &-- & \\ CaI & 6166.440 & 2.52 & 3.97E-31$^{aa}$ & --0.90$^1$ & --1.156& +0.20 & +0.0 & +0.1 & 78.2 &104.2 & \\ CaI & 6169.044 & 2.52 & 3.97E-31$^{aa}$ & --0.54$^1$ & --0.90 & +0.10 & +0.0 & +0.1 & 72.6 & 105.4 & \\ CaI & 6169.564 & 2.52 & 4.0E-31$^{aa}$ & --0.27$^1$ & --0.63 & +0.10 & +0.0 & +0.1 & 98.0 &-- & \\ CaI & 6439.080 & 2.52 & 3.4E-32$^{aa}$ & +0.3$^4$ & +0.3 & +0.00 & +0.0 & +0.1: & 166.5 & -- & \\ CaI & 6455.605 & 2.52 & 3.39E-32$^{aa}$ & --1.35$^1$ & --1.55 & +0.10 & +0.0:& -- & 55.2 & -- & \\ CaI & 6464.679 & 2.52 & 3.4E-32$^{aa}$ & --2.10$^2$ & --2.48 & +0.40 & -- & -- &-- & -- & \\ CaI & 6471.668 & 2.52 & 3.39E-32$^{aa}$ & --0.59$^1$ & --0.80 & +0.00 & --0.1 & +0.1 & 74.0 & 95.6 & \\ CaI & 6493.788 & 2.52 & 3.37E-32$^{aa}$ & +0.14$^1$ & 0.0 & --0.15 & --0.1 & --0.1 & 141.0 &146.9 & \\ CaI & 6499.654 & 2.52 & 3.37E-32$^{aa}$ & --0.59$^1$ & --0.85 & --0.15 & --0.1 & +0.1 & 81.0 &110.9 & \\ CaI & 6508.846 & 2.52 & 3.37E-32$^{aa}$ & --2.50$^3$ & --2.51 & +0.10 & -- & -- & -- &-- & \\ CaI & 6572.779 & 0.00 & 1.75E-32$^{aa}$ & --4.29$^1$ & --4.32 & +0.10 & --0.1 & +0.1 & 63.4 & 111.3& \\ CaI & 6717.687 & 2.71 & 4.1E-31$^{aa}$ & --0.61$^1$ & --0.61 & +0.10 & --0.1 &+0.1 & -- & 131.9 & \\ % TiI & 5866.452 & 1.07 & 1.44E-32$^{aa}$ & --0.84$^1$ & --0.84 & +0.1 & +0.0 & +0.0 & 80.5 & 109.5 & \\ TiI & 5922.110 & 1.05 & 2.32E-32$^{aa}$ & --1.47$^1$ & --1.50 & +0.1 & +0.1 & +0.0 & 56.3 & 66.8 & \\ TiI & 5965.835 & 1.88 & 2.14E-32$^{a}$ & --0.41$^1$ & --0.45 & +0.1 & +0.1 & +0.0 &48.4 &77.3 & \\ TiI & 5978.549 & 1.87 & 1.43E-32$^{aa}$ & --0.50$^1$ & --0.55 & +0.1 & +0.1 & +0.0 &27.4 &52.4 & \\ TiI & 6064.626 & 1.05 & 1.37E-32$^{aa}$ & --1.94$^1$ & --1.94 & +0.1 & -- & -- &-- & -- & \\ TiI & 6091.177 & 2.27 & 2.59E-32$^{aa}$ & --0.42$^1$ & --0.42 & +0.0 & +0.1 & +0.0 & 18.1 & 45.7 & \\ TiI & 6126.224 & 1.07 & 1.37E-32$^{aa}$ & --1.43$^1$ & --1.43 & +0.0 & +0.0 & +0.0: & 50.0 & 68.3 & \\ TiI & 6258.110 & 1.44 & 3.17E-32$^{aa}$ & --0.36$^1$ & --0.36 & +0.1 & --0.1 & +0.0 & 63.5 & 113.2 & \\ TiI & 6261.106 & 1.43 & 4.68E-32$^{a}$ & --0.48$^1$ & --0.48 & +0.1 & +0.1 & +0.0 & 91.3 & 120.9 & \\ TiI & 6303.767 & 1.44 & 3.12E-32$^{aa}$ & --1.57$^1$ & --1.57 & +0.1 & +0.1 & +0.1 & 16.1 & 40.6 & \\ TiI & 6312.238 & 1.46 & 3.17E-32$^{aa}$ & --1.69$^1$ & --1.69 & +0.2:& +0.1 & +0.0 & -- & 31.2 & \\ TiI & 6336.113 & 1.44 & 1.86E-32$^{aa}$ & --1.74$^1$ & --1.74 & +0.1 & -- & +0.1: & 22.2 &32.8 & \\ TiI & 6508.154 & 1.43 & 1.46E-32$^{a}$ & --2.05$^3$ & --2.05 & +0.1 & -- & +0.0: & -- &10.9 & \\ TiI & 6554.238 & 1.44 & 1.81E-32$^{aa}$ & --1.22$^1$ & --1.22 & +0.1 & --0.1 & +0.0 & 22.7 & 67.3 & \\ TiI & 6556.077 & 1.46 & 1.81E-32$^{aa}$ & --1.07$^1$ & --1.07 & +0.1 & +0.1 & +0.0 & 41.3 & 68.6 & \\ TiI & 6599.113 & 0.90 & 1.96E-32$^{aa}$ & --2.09$^1$ & --2.09 & +0.1 & +0.1 & +0.0 & 20.8 & 55.1 & \\ \hline TiI & 6743.127 & 0.90 & 0.30E-31 & --1.63$^1$ & --1.73 & +0.1 & --0.2 & +0.0 & 32.9 & 79.7 & \\ TiII& 6491.580 & 2.06 & 0.30E-31 & --2.10$^{1*}$ & --2.10 & +0.1 & +0.1 & +0.3: & 73.2 & 79.1 & \\ TiII& 6559.576 & 2.05 & 0.30E-31 & --2.48$^3$ & --2.35 & +0.1 & -- & +0.1 & -- & 5.4 & \\ TiII& 6606.970 & 2.06 & 0.30E-31 & --2.79$^1$ & --2.85 & +0.1 & +0.1 & +0.0 & 22.9 & 22.9 & \\ BaII & 6141.727 & 0.70 & & hfs & hfs & --0.20 & +0.2 & +0.2 & 158.1 & 162.1 & \\ BaII & 6496.908 & 0.60 & & hfs & hfs & --0.20 & +0.0 & +0.2 & 192.0 & 179.6 & \\ LaII & 6390.480 & 0.32 & & hfs & hfs & --0.30 & 0.0 & +0.0 & 18.0 & 20.3 & \\ EuII & 6645.127 & 1.38 & & hfs & hfs & +0.30 & +0.0 & +0.3 & 17.4 & 31.9 \\ \hline \end{tabular} \medskip $^a$ Damping constants computed following Barklem et~al. (\cite{Barklem98}, \cite{Barklem00}); $^{aa}$ damping constants computed as in $^a$, decreased by a factor 1.5~($C_6$/1.5). Other $C_6$ values are van der Waals classical ones, as described in Zoccali et~al. (\cite{Zoccali04}). Column 5 reports the log~$gf$ used in Zoccali et~al. (\cite{Zoccali04}), adopted from $^1$ NIST/VALD; $^2$ Barbuy et~al. (1999); $^3$ McWilliam \& Rich (\cite{McWilliam94}); $^4$ Bensby et~al. (2004), whereas Col.~6 gives the values derived in this work from a fit to the solar spectrum; $^*$ for TiII 6491.58 ${\rm \AA}$ line, the NIST log~$gf$~= $-2.10$ is different from the VALD value of log~$gf$~=~$-1.793$. \end{table}