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Table 1:

Basic data.

RA Dec z $L_{\rm X,bol}$a kT M500b R500 $R_{\rm det}$c
        (erg s-1) (keV) $(\times 10^{13}~M_{\odot})$ (kpc) (R500)

RXC J0216.7-4749
$02^{\rm h} 16^{\rm m} 45\hbox{$.\!\!^{\rm s}$ }0$ $-47\hbox{$^\circ$ }49\hbox{$^\prime$ }09\hbox{$.\!\!^{\prime\prime}$ }8$ 0.064 $3.2 \times 10^{43}$ $2.05\pm0.05$ $8.14\pm0.16$ $645.7\pm5.0$ 1.0
RXC J2315.7-0222 $23^{\rm h} 15^{\rm m} 44\hbox{$.\!\!^{\rm s}$ }4$ $-02\hbox{$^\circ$ }22\hbox{$^\prime$ }54\hbox{$.\!\!^{\prime\prime}$ }4$ 0.026 $2.1 \times 10^{43}$ $1.68\pm0.03$ $5.36\pm0.37$ $568.7\pm13.1$ 0.73

Notes. (a) Bolometric ([0.001-100.] keV) luminosity calculated assuming $\Omega_M = 1$, $\Omega_\Lambda = 0$ and h0 = 0.5; (b) estimated from the M500-YX relation of Arnaud et al. (2007); (c) ratio of the weighted effective radius of the final bin of the temperature profile,  $R_{\rm det}$, to R500.

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