\begin{table}%tC.1
\caption{\label{tab:pnfw}Cluster physical parameters.}
\par
%\centering
\par
\begin{tabular}{lccccccccccc}
\hline \hline \noalign{\smallskip}
    Cluster &  $\Rv $ & $Y_{\rm X}$ & $Y_{\rm sph}(R_{2500})$ &  $Y_{\rm sph}(\Rv)$ & $P_{500}$ & $P_0$&$c_{500}$ & $\alpha$ & $\gamma$ &$\chi^2/{\rm d.o.f.}$\\
     & (Mpc) & $(10^{14}~\msol~\keV)$ & $(10^{-5}~{\rm Mpc^2})$ &$(10^{-5}~{\rm Mpc^2})$& $(10^{-3}~\keV~{\rm cm}^{-3})$ & \\
    \hline
RXC J0003.8+0203 & $ 0.879$ & $ 0.763\pm0.030$ & $ 0.410\pm0.009$ & $ 0.990\pm0.036$ & $ 1.466$ & $ 3.93$ & $1.33$ & $1.41$ & $0.567 $ & $0.3/9$ \\
RXC J0006.6-3443 & $ 1.075$ & $ 2.35\pm0.13$ & $ 1.030\pm0.050$ & $ 3.06\pm0.16$ & $ 2.292$ & $ 3.27$ & $1.10$ & $1.41$ & $0.408 $ & $0.0/1$ \\
RXC J0020.7-2542 & $ 1.056$ & $ 2.253\pm0.072$ & $ 1.419\pm0.034$ & $ 2.80\pm0.11$ & $ 2.331$ & $ 20.26$ & $2.16$ & $1.37$ & $0.035 $ & $3.7/7$ \\
RXC J0049.4-2931 & $ 0.800$ & $ 0.477\pm0.022$ & $ 0.277\pm0.010$ & $ 0.630\pm0.037$ & $ 1.254$ & $ 8.58$ & $1.31$ & $1.07$ & $0.422 $ & $0.2/4$ \\
RXC J0145.0-5300 & $ 1.112$ & $ 2.819\pm0.097$ & $ 1.193\pm0.029$ & $ 3.89\pm0.18$ & $ 2.461$ & $ 9.73$ & $1.06$ & $1.06$ & $0.000 $ & $1.1/4$ \\
RXC J0211.4-4017 & $ 0.684$ & $ 0.203\pm0.006$ & $ 0.101\pm0.003$ & $ 0.267\pm0.010$ & $ 0.902$ & $ 8.97$ & $1.04$ & $0.93$ & $0.267 $ & $3.0/6$ \\
RXC J0225.1-2928 & $ 0.683$ & $ 0.185\pm0.014$ & $ 0.087\pm0.004$ & $ 0.237\pm0.017$ & $ 0.832$ & $ 19.28$ & $1.19$ & $0.88$ & $0.000 $ & $5.4/5$ \\
RXC J0345.7-4112 & $ 0.685$ & $ 0.188\pm0.009$ & $ 0.109\pm0.003$ & $ 0.227\pm0.009$ & $ 0.836$ & $ 3.68$ & $1.65$ & $1.67$ & $0.690 $ & $1.1/7$ \\
RXC J0547.6-3152 & $ 1.148$ & $ 3.59\pm0.11$ & $ 1.976\pm0.037$ & $ 4.54\pm0.14$ & $ 2.799$ & $ 8.52$ & $1.74$ & $1.51$ & $0.260 $ & $3.8/6$ \\
RXC J0605.8-3518 & $ 1.059$ & $ 2.285\pm0.070$ & $ 1.264\pm0.025$ & $ 3.13\pm0.14$ & $ 2.338$ & $ 4.23$ & $0.88$ & $0.96$ & $0.659 $ & $1.1/6$ \\
RXC J0616.8-4748 & $ 0.947$ & $ 1.194\pm0.044$ & $ 0.515\pm0.014$ & $ 1.627\pm0.060$ & $ 1.784$ & $ 4.06$ & $1.16$ & $1.43$ & $0.234 $ & $1.4/3$ \\
RXC J0645.4-5413 & $ 1.302$ & $ 7.291\pm0.248$ & $ 3.60\pm0.11$ & $ 9.93\pm0.47$ & $ 3.722$ & $ 11.10$ & $0.94$ & $0.89$ & $0.265 $ & $2.5/5$ \\
RXC J0821.8+0112 & $ 0.753$ & $ 0.325\pm0.017$ & $ 0.171\pm0.007$ & $ 0.400\pm0.019$ & $ 1.053$ & $ 1.72$ & $1.37$ & $2.01$ & $0.860 $ & $1.5/1$ \\
RXC J0958.3-1103 & $ 1.076$ & $ 2.64\pm0.25$ & $ 1.72\pm0.11$ & $ 3.42\pm0.40$ & $ 2.553$ & $ 4.13$ & $1.77$ & $2.07$ & $0.719 $ & $0.0/3$ \\
RXC J1044.5-0704 & $ 0.939$ & $ 1.189\pm0.024$ & $ 0.732\pm0.010$ & $ 1.550\pm0.051$ & $ 1.820$ & $ 7.08$ & $1.27$ & $1.05$ & $0.644 $ & $13.7/7$ \\
RXC J1141.4-1216 & $ 0.893$ & $ 0.879\pm0.018$ & $ 0.491\pm0.007$ & $ 1.199\pm0.046$ & $ 1.597$ & $ 4.42$ & $1.08$ & $1.08$ & $0.652 $ & $15.3/6$ \\
RXC J1236.7-3354 & $ 0.758$ & $ 0.335\pm0.011$ & $ 0.162\pm0.003$ & $ 0.479\pm0.020$ & $ 1.062$ & $ 47.76$ & $0.72$ & $0.61$ & $0.000 $ & $3.2/4$ \\
RXC J1302.8-0230 & $ 0.850$ & $ 0.625\pm0.020$ & $ 0.305\pm0.007$ & $ 0.800\pm0.039$ & $ 1.349$ & $ 3.63$ & $1.09$ & $1.21$ & $0.519 $ & $14.8/6$ \\
RXC J1311.4-0120 & $ 1.351$ & $ 9.27\pm0.17$ & $ 5.610\pm0.084$ & $ 11.60\pm0.30$ & $ 4.169$ & $ 23.13$ & $1.16$ & $0.78$ & $0.399 $ & $17.1/7$ \\
RXC J1516+0005 & $ 1.010$ & $ 1.689\pm0.050$ & $ 0.927\pm0.013$ & $ 2.211\pm0.083$ & $ 2.035$ & $ 4.48$ & $1.52$ & $1.65$ & $0.474 $ & $4.1/5$ \\
RXC J1516.5-0056 & $ 0.932$ & $ 1.105\pm0.038$ & $ 0.479\pm0.015$ & $ 1.494\pm0.054$ & $ 1.740$ & $ 2.57$ & $1.09$ & $1.51$ & $0.465 $ & $1.2/4$ \\
RXC J2014.8-2430 & $ 1.176$ & $ 4.133\pm0.097$ & $ 2.293\pm0.056$ & $ 5.59\pm0.23$ & $ 2.971$ & $ 4.94$ & $0.75$ & $0.82$ & $0.684 $ & $8.8/7$ \\
RXC J2023.0-2056 & $ 0.740$ & $ 0.281\pm0.014$ & $ 0.149\pm0.005$ & $ 0.358\pm0.016$ & $ 0.968$ & $ 4.00$ & $1.36$ & $1.41$ & $0.515 $ & $0.2/2$ \\
RXC J2048.1-1750 & $ 1.095$ & $ 2.782\pm0.084$ & $ 1.104\pm0.024$ & $ 3.73\pm0.12$ & $ 2.542$ & $ 4.34$ & $1.33$ & $1.76$ & $0.000 $ & $10.7/3$ \\
RXC J2129.8-5048 & $ 0.903$ & $ 0.856\pm0.043$ & $ 0.357\pm0.016$ & $ 1.147\pm0.051$ & $ 1.508$ & $ 9.21$ & $0.94$ & $1.00$ & $0.000 $ & $0.2/0$ \\
RXC J2149.1-3041 & $ 0.891$ & $ 0.864\pm0.024$ & $ 0.429\pm0.009$ & $ 1.135\pm0.051$ & $ 1.585$ & $ 9.96$ & $0.71$ & $0.71$ & $0.446 $ & $3.3/6$ \\
RXC J2157.4-0747 & $ 0.753$ & $ 0.311\pm0.012$ & $ 0.122\pm0.005$ & $ 0.411\pm0.015$ & $ 1.007$ & $ 1.46$ & $1.24$ & $2.54$ & $0.491 $ & $0.1/1$ \\
RXC J2217.7-3543 & $ 1.031$ & $ 2.023\pm0.050$ & $ 1.079\pm0.021$ & $ 2.611\pm0.077$ & $ 2.260$ & $ 27.70$ & $1.18$ & $0.81$ & $0.133 $ & $0.2/5$ \\
RXC J2218.6-3853 & $ 1.147$ & $ 3.51\pm0.14$ & $ 1.796\pm0.049$ & $ 4.94\pm0.29$ & $ 2.751$ & $ 27.29$ & $1.06$ & $0.82$ & $0.000 $ & $1.0/4$ \\
RXC J2234.5-3744 & $ 1.307$ & $ 7.22\pm0.17$ & $ 4.300\pm0.075$ & $ 8.82\pm0.25$ & $ 3.647$ & $ 25.04$ & $2.01$ & $1.23$ & $0.000 $ & $10.6/5$ \\
RXC J2319.6-7313 & $ 0.793$ & $ 0.445\pm0.018$ & $ 0.194\pm0.004$ & $ 0.612\pm0.026$ & $ 1.207$ & $ 338.9$ & $0.17$ & $0.33$ & $0.065 $ & $1.9/5$ \\
\hline                                    
\end{tabular}
\tablefoot {Columns (2),~(3): $\Rv$ is the radius corresponding to a density contrast of~500,  estimated iteratively from the \MY~relation (Eq.~(\ref{eq:mynstd})), where $Y_{\rm X}=\Mgv\TX$ is the product of the gas mass within $\Rv$ and the spectroscopic temperature~$\TX$.   Columns~(4) and~(5): spherically integrated Compton parameter within $R_{2500}$ and~$\Rv$, respectively. Column~(6):  $P_{500}$~as defined by Eq.~(\ref{eq:p500}). Columns~(7) to~(10)  give the best fitting GNFW~parameters for the pressure profiles (Eq.~(\ref{eq:pgnfw})). The external slope parameter~$\beta$ has been fixed to~$5.49$ (see~text). Redshift~$z$ and $\Mv$~values can be found in Table~\ref{tab:rellx} of \citet{pra10}.}
\end{table}