\begin{table}%t5
 \small  \caption{RR: partial results. We list the mean $\mu$ and the
    corresponding standard deviation $\sigma$ of the difference
  Committee-SSPP for each of the different stellar types and parameter
  ranges.}\label{t_Partial1RR}
    %\begin{center}
\par
    \leavevmode
        \begin{tabular}[h]{ccrrrrrrrrr} 
        \hline\hline  
        ${\rm [Fe/H]}$ & $\log~T_{\rm eff}$ & 
        $\mu_{\log~T_{\rm eff}}$&$\sigma_{\log~T_{\rm eff}}$&$E_{\log~T_{\rm eff}}$ &
        $\mu_{\log~g}$&$\sigma_{\log~g}$&$E_{\log~g}$&
        $\mu_{\rm [Fe/H]}$&$\sigma_{\rm [Fe/H]}$& $E_{\rm [Fe/H]}$\\ 
        \hline  
$<$$-1.5$ & $<$$3.70$ & $0.0155$ & $0.0166$ & $0.0172$ & $0.1879$ & $0.4448$ & $0.3724$ & $0.2673$ & $0.2733$ & $0.3056$\\
$<$$-1.5$ & $3.70,3.75$ & $0.0061$ & $0.0134$ & $0.0105$ & $0.1214$ & $0.3939$ & $0.3075$ & $0.0817$ & $0.2072$ & $0.1464$\\
$<$$-1.5$ & $3.75,3.80$ & $0.0011$ & $0.0097$ & $0.0073$ & $0.1284$ & $0.3463$ & $0.2823$ & $0.0619$ & $0.1531$ & $0.1266$\\
$<$$-1.5$ & $3.80,3.85$ & $-0.0032$ & $0.0107$ & $0.0082$ & $-0.1141$ & $0.4439$ & $0.3606$ & $0.0305$ & $0.2048$ & $0.1484$\\
$<$$-1.5$ & $3.85,3.875$ & $0.0146$ & $0.0128$ & $0.0167$ & $0.1617$ & $0.5463$ & $0.4117$ & $0.1070$ & $0.3837$ & $0.2882$\\
$<$$-1.5$ & $>$$3.875$ & $-0.0044$ & $0.0230$ & $0.0173$ & $0.0007$ & $0.3487$ & $0.2412$ & $0.2860$ &$0.4164$ & $0.3875$\\ 
\hline  
$>$$-1.5$ & $<$$3.70$ & $0.0087$ & $0.0129$ & $0.0118$ & $0.0941$ & $0.3696$ & $0.2882$ & $0.0295$ & $0.2150$ & $0.1658$\\
$>$$-1.5$ & $3.70,3.75$ & $0.0010$ & $0.0112$ & $0.0083$ & $0.0206$ & $0.3187$ & $0.2466$ & $0.0078$ & $0.1403$ & $0.1044$\\
$>$$-1.5$ & $3.75,3.80$ & $-0.0034$ & $0.0107$ & $0.0084$ & $-0.0765$ & $0.3051$ & $0.2458$ & $-0.0359$ & $0.1469$ & $0.1139$\\
$>$$-1.5$ & $3.80,3.85$ & $-0.0052$ & $0.0127$ & $0.0097$ & $-0.0698$ & $0.4512$ & $0.3462$ & $-0.0923$ & $0.2307$ & $0.1904$\\
$>$$-1.5$ & $3.85,3.875$ & $0.0022$ & $0.0105$ & $0.0081$ & $-0.0786$ & $0.5434$ & $0.4127$ & $-0.0484$ & $0.2511$ & $0.1898$\\
$>$$-1.5$ & $>$$3.875$ & $-0.0119$ & $0.0189$ & $0.0151$ & $-0.0361$ & $0.4226$ & $0.3085$ & $-0.2144$ & $0.3799$ & $0.3226$\\ 
\hline\hline 
        $\log~g$ & $\log~T_{\rm eff}$ & 
        $\mu_{\log~T_{\rm eff}}$&$\sigma_{\log~T_{\rm eff}}$&$E_{\log~T_{\rm eff}}$ &
        $\mu_{\log~g}$&$\sigma_{\log~g}$&$E_{\log~g}$&
        $\mu_{\rm [Fe/H]}$&$\sigma_{\rm [Fe/H]}$& $E_{\rm [Fe/H]}$\\ 
        \hline  
$<$$3.5$ & $<$$3.70$ & $0.0193$ & $0.0164$ & $0.4302$ & $0.3427$ & $0.4407$ & $0.4302$ & $0.1685$ & $0.2540$ & $0.2347$\\
$<$$3.5$ & $3.70,3.75$ & $0.0060$ & $0.0150$ & $0.3577$ & $0.2045$ & $0.4069$ & $0.3577$ & $0.0518$ & $0.1950$ & $0.1454$\\
$<$$3.5$ & $3.75,3.80$ & $0.0034$ & $0.0112$ & $0.4115$ & $0.3747$ & $0.3202$ & $0.4115$ & $0.0687$ & $0.1719$ & $0.1401$\\
$<$$3.5$ & $3.80,3.85$ & $0.0018$ & $0.0128$ & $0.6220$ & $0.6182$ & $0.3584$ & $0.6220$ & $0.0516$ & $0.2630$ & $0.1946$\\
$<$$3.5$ & $3.85,3.875$ & $0.0122$ & $0.0139$ & $0.5691$ & $0.5357$ & $0.5020$ & $0.5691$ & $0.1258$ & $0.2992$ & $0.2347$\\
$<$$3.5$ & $>$$3.875$ & $-0.0078$ & $0.0240$ & $0.2639$ & $0.1860$ & $0.3137$ & $0.2639$ & $0.0662$ & $0.4635$ & $0.3435$\\ 
\hline 
$>$$3.5$ & $<$$3.70$ & $0.0069$ & $0.0114$ & $0.0105$ & $0.0438$ & $0.3373$ & $0.2644$ & $0.0294$ & $0.2226$ & $0.1692$\\
$>$$3.5$ & $3.70,3.75$ & $0.0001$ & $0.0099$ & $0.0075$ & $-0.0207$ & $0.2805$ & $0.2216$ & $0.0024$ & $0.1287$ & $0.0968$\\
$>$$3.5$ & $3.75,3.80$ & $-0.0035$ & $0.0100$ & $0.0080$ & $-0.1172$ & $0.2509$ & $0.2188$ & $-0.0300$ & $0.1434$ & $0.1116$\\
$>$$3.5$ & $3.80,3.85$ & $-0.0054$ & $0.0116$ & $0.0091$ & $-0.2033$ & $0.3408$ & $0.3051$ & $-0.0641$ & $0.2185$ & $0.1717$\\
$>$$3.5$ & $3.85,3.875$ & $0.0019$ & $0.0099$ & $0.0076$ & $-0.2488$ & $0.3877$ & $0.3497$ & $-0.0700$ & $0.2675$ & $0.2005$\\
$>$$3.5$ & $>$$3.875$ & $-0.0092$ & $0.0190$ & $0.0146$ & $-0.1452$ & $0.3797$ & $0.2874$ & $-0.0367$ & $0.4618$ & $0.3521$\\ 
\hline  
       \end{tabular}
  %\end{center}
\par
\end{table}