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Table 1:

Main properties of clusters in our sample.

ID
$\alpha$ (J2000) $\delta$ (J2000) z LX r200
        (10-37 W) (Mpc)

MS 0015.9+1609
00:18:33.33 +16:26:44.6 0.54 [2] 15.5 [2] 2.11 [3]
MS 0451.5-0305 04:54:10.796 -03:00:53.0 0.54 [2] 23.7 [2] 1.47 [3]
MS 1621.5+2640 16:23:35.6277 +26:34:09.49 0.43 [2] 9.47 [2] 1.5 [3]
MS1241.5+1710 12:44:01.4 +16:53:42 0.55 [2] 1.73 [2] 1.7 [3]
RXC J0856.1+3756 08:56:08.5 +37:56:52 0.41 [1] 15.76 [1] 1.59 [3]
RX J1003.0+3757 10:03:02.74 +37:57:51.5 0.41 [1] 8.29 [1] 1.48 [3]
RX J1120+4318 11:20:07.5 +43:18:05 0.60 [2] 6.07 [2] 1.3 [3]
RXC J1206.2-0848 12:06:13.1 -08:47:43 0.44 - 2.0 [3]
RXC J2228.6+2036 22:28:37.1 +20:36:31 0.41 [1] 29.62 [1] 1.62 [3]
[1] Böhringer et al. (2000); [2] Sadat et al. (2004); [3] Foex et al. 2009, in prep. r200 are computed through a 1D weak-lensing analysis, i.e. fit of the radial shear profile and are defined as the radius at which the density is 200 times the critical density of the Universe at the cluster redshift.

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