\begin{table}%t5
\caption{\label{T5}Quasi-periodic decomposition of the resonant angle
$\theta = 2 \lambda_b - \lambda_c - \varpi_2^*$ for an integration  over 100~kyr of the orbital solution in   Table~\ref{T2}.} 
%\centering
 \begin{tabular}{rrrrrrrr}
\hline\hline \noalign{\smallskip}
\multicolumn{5}{c}{Combination} & $\nu_i$ & $A_i$  & $\phi_i$  \\
$n_b$ & $n_c$ & $g_2$&$g_3$&  $l_\theta$ & (deg/yr) & (deg) & (deg) \\
\hline
0 &  0 &   0  &  0 &    1 &      245.9180 &         1.810 &      --48.681 \\ 
1 &  1 &  --2  &  0 &    0 &     6586.5572 &         0.567 &       96.286 \\ 
0 &  1 &  --1  &  0 &    0 &     2195.5191 &         0.569 &       32.095 \\ 
0 &  0 &  --1  &  1 &    0 &       41.7516 &         0.411 &      --94.109 \\ 
1 &  0 &  --1  &  0 &    0 &     4391.0382 &         0.255 &      --25.809 \\ 
2 &  1 &  --3  &  0 &    0 &    10977.5954 &         0.156 &      --19.523 \\ 
 0 &  0 &   1  & -1 &    1 &      204.1664 &         0.120 &      --44.572 \\ 
  \hline
\end{tabular}
\tablefoot{We have $\theta = \sum_{i=1}^N A_i \cos(\nu_i~ t + \phi_i)$. 
  We only provide the first 7~largest terms that are identified as
  integer combinations    of the fundamental frequencies given in
  Table~\ref{T4}. }
  \label{Tj5}\vspace{-2mm}
\end{table}