\begin{table}%t1
\caption{\label{table:1}The values of fitting parameters, defined in Eq.~(3),
 for proton excitation rate coefficients of transitions in ions Fe X--Fe XV.}      
%\centerline
{\begin{tabular}{c c c c c c c c c c c c}     % 12 columns 
\hline\hline \noalign{\smallskip}       
Ref. & Ion & Transition & $p_1$ (cm$^3$s$^{-1}$) & $p_2$ (eV) & $p_3$ & $p_4$ (eV) & $p_5$ & $p_6$ (eV) & $p_7$ & Accuracy (\%)  & $T_{\rm p}$ (eV)  \\    % table heading 
\hline \noalign{\smallskip}                   
1 & X & $\rm 3s^23p^5\ ^2P_{3/2}{-}3s^23p^5\ ^2P_{1/2}$ & 2.99 & 47 & 1.4 & 87 & 2.4 & 38 & 2.3 & 1.2 & 20--400\\
2 & X & $\rm 3s^23p^5\ ^2P_{3/2}{-}3s^23p^5\ ^2P_{1/2}$ & 3.03 & 47 & 1.4 & 83 & 1.9 & 38 & 2.3 & 1.5 & 20--400\\
3 & XI & $\rm 3s^23p^4\ ^3P_2{-}3s^23p^4\ ^3P_1$ & 6.05 & 55 & 1.5 & 270 & 1.36 & 79 & 1.3 & 1.9 & 20--250\\
3 & XI & $\rm 3s^23p^4\ ^3P_2{-}3s^23p^4\ ^3P_0$ & 1.485 & 55 & 1.5 & 310 & 2.9 & 79 & 1.4 & 2.0 & 20--250\\
3 & XI & $\rm 3s^23p^4\ ^3P_1{-}3s^23p^4\ ^3P_0$ & 0.0126 & 55 & 1.5 & 192 & 2.18 & 11 & 2 & 2.4 & 20--250\\
4 & XII & $\rm 3s^23p^3\ ^4S_{3/2}{-}3s^23p^3\ ^2D_{3/2}$ & 0.01   &  71 & 3 & 110 & 1.1 & 50 & 2 & 1.5 & 70--250\\
4 & XII & $\rm 3s^23p^3\ ^4S_{3/2}{-}3s^23p^3\ ^2D_{5/2}$ & 0.017   &  74 & 3 & 107 & 1.1 & 49 & 2 & 1.6 & 70--250\\
4 & XII & $\rm 3s^23p^3\ ^4S_{3/2}{-}3s^23p^3\ ^2P_{1/2}$ & 0.00028   & 82.5 & 3 & 3000 & 1.1 & 49 & 2 & 2.4 & 70--250\\
4 & XII & $\rm 3s^23p^3\ ^4S_{3/2}{-}3s^23p^3\ ^2P_{3/2}$ & 0.0007   &  81 & 3 & 530 & 1.1 & 50 & 2 & 3.0 & 70--250\\
4 &  XII & $\rm 3s^23p^3\ ^2D_{3/2}{-}3s^23p^3\ ^2D_{5/2}$ & 0.3 & 38 & 3 & 550 & 1.1 & 50 & 1 & 1.7 & 70--250\\
4 &  XII & $\rm 3s^23p^3\ ^2D_{3/2}{-}3s^23p^3\ ^2P_{1/2}$ & 0.02 & 76 & 3 & 1500 & 1.1 & 50 & 2 & 1.2 & 70--250\\
4 &  XII & $\rm 3s^23p^3\ ^2D_{3/2}{-}3s^23p^3\ ^2P_{3/2}$ & 0.025 & 74 & 3 & 400 & 1.1 & 50 & 2 & 1.4 & 70--250\\
4 &  XII & $\rm 3s^23p^3\ ^2D_{5/2}{-}3s^23p^3\ ^2P_{1/2}$ & 0.0202 & 70.7 & 3 & 343 & 1.1 & 50 & 2 & 3.0 & 70--250\\
4 &  XII & $\rm 3s^23p^3\ ^2D_{5/2}{-}3s^23p^3\ ^2P_{3/2}$ & 0.0598 & 70.7 & 3 & 328 & 1.1 & 50 & 2 & 1.0 & 70--250\\
4 &  XII & $\rm 3s^23p^3\ ^2P_{1/2}{-}3s^23p^3\ ^2P_{3/2}$ & 0.3 & 49.8 & 4 & 119 & 1.8 & 50 & 2 & 0.7 & 70--250\\
5 &  XIII & $\rm 3s^23p^2\ ^3P_0{-}3s^23p^2\ ^3P_1$ & 0.185 & 65 & 3 & 345 & 1.7 & 45 & 2 & 1.1 & 60--270\\
5 &  XIII & $\rm 3s^23p^2\ ^3P_0{-}3s^23p^2\ ^3P_2$ & 1.23 & 62 & 3 & 210 & 1.7 & 45 & 2 & 0.6 & 60--270\\
5 &  XIII & $\rm 3s^23p^2\ ^3P_0{-}3s^23p^2\ ^1D_2$ & 0.3 & 73.2 & 3.5 & 174 & 1.85 & 46.6 & 2 & 1.6 & 60--270\\
5 &  XIII & $\rm 3s^23p^2\ ^3P_0{-}3s^23p^2\ ^1S_0$ & 0.00005 & 64 & 3.5 & 450 & 2 & 30 & 3 & 1.1 & 60--270\\
5 &  XIII & $\rm 3s^23p^2\ ^3P_1{-}3s^23p^2\ ^3P_2$ & 1.98 & 38 & 3 & 160 & 1.9 & 45 & 2 & 1.0 & 60--270\\
5 &  XIII & $\rm 3s^23p^2\ ^3P_1{-}3s^23p^2\ ^1D_2$ & 0.106 & 65.5 & 3 & 258 & 2.4 & 45 & 2 & 0.8 & 60--270\\
5 &  XIII & $\rm 3s^23p^2\ ^3P_1{-}3s^23p^2\ ^1S_0$ & 0.00005 & 75 & 3.7 & 280 & 2.4 & 29.7 & 3 & 1.2 & 60--270\\
5 &  XIII & $\rm 3s^23p^2\ ^3P_2{-}3s^23p^2\ ^1D_2$ & 0.365 & 64 & 3 & 208 & 1.7 & 45 & 2 & 1.2 & 60--270\\
5 &  XIII & $\rm 3s^23p^2\ ^3P_2{-}3s^23p^2\ ^1S_0$ & 0.000256 & 79 & 3 & 320 & 2.2 & 27.2 & 3 & 1.8 & 60--270\\
5 &  XIII & $\rm 3s^23p^2\ ^1D_2{-}3s^23p^2\ ^1S_0$ & 0.00512 & 74 & 2.6 & 280 & 2.2 & 27.2 & 3 & 0.8 & 60--270\\
5 &  XIV & $\rm 3s^23p\ ^2P_{1/2}{-}3s^23p\ ^2P_{3/2}$ & 1.03 & 72.6 & 1.3 & 125 & 1.8 & 28.7 & 2.1 & 1.6 & 20--500\\
6 &  XV & $\rm 3s3p\ ^3P_0{-}3s3p\ ^3P_1$ & 0.0499 & 78 & 2.5 & 365 & 2 & 65 & 2 & 1.4 & 70--900\\
6 &  XV & $\rm 3s3p\ ^3P_0{-}3s3p\ ^3P_2$ & 0.0986 & 60 & 3 & 224 & 2 & 48 & 2.1 & 2.4 & 70--900\\
6 &  XV & $\rm 3s3p\ ^3P_1{-}3s3p\ ^3P_2$ & 0.1 & 51 & 3 & 225 & 2 & 50 & 2.1 & 1.9 & 70--900\\
\hline                  
\end{tabular}}
\par
\tablebib{(1) Kastner \& Bhatia (\cite{Kastner1979}); (2) Bely \& Faucher (\cite{Bely1970}); (3) Landman (\cite{Landman1980}); (4) Landman (\cite{Landman1978}); (5) Landman (\cite{Landman1975}); (6) Landman \& Brown (\cite{Landman1979}).}
\end{table}