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Table 1

Data for the clusters with usable XMM-Newton data.

Name RA Dec z Nz Δt (s) kT (keV) LX (erg s-1) Mgas,r500 (M) Mtot,r500 (M) Substructure

CL 0016+1609 4.63888 16.44329 0.5455 173 30320 8.97 ± 0.40 2.23 ± 0.06e+45 1.17 ± 0.03e+14 1.24 ± 0.04e+15 1
CL J0152.7-1357 28.17083 –13.96250 0.8310 115 51150 7.55 ± 0.65 7.91 ± 0.74e+44 7.72 ± 0.28e+13 8.83 ± 0.38e+14 1
MS 0302.5+1717 46.32911 17.47729 0.4250 1 12440 6.23 ± 1.13 1.41 ± 0.35e+44 6.02 ± 0.72e+13 6.84 ± 0.67e+14 0/–1
XDCS cm J032903.1+025640 52.26175 2.94033 0.4122 13 47520 3.26 ± 0.38 1.40 ± 0.89e+43 2.60 ± 0.30e+13 2.88 ± 0.40e+14 –1
RX J0337.6-2522 54.43812 –25.37669 0.5850 5 11820 2.40 ± 0.78 5.73 ± 4.98e+43 1.65 ± 0.25e+13 1.85 ± 0.36e+14 0
MACS J0454.1-0300 73.54552 –3.01865 0.5377 194 25420 9.97 ± 0.59 2.04 ± 0.06e+45 1.29 ± 0.04e+14 1.39 ± 0.04e+15 1
BMW-HRI J052215.8-362452 80.55917 –36.41778 0.4720 1 17920 5.64 ± 0.66 1.70 ± 0.27e+44 4.99 ± 0.32e+13 5.78 ± 0.41e+14 0/–1
MACS J0647.7+7015 101.94125 70.25083 0.5907 1 32030 7.74 ± 0.35 1.61 ± 0.07e+45 9.76 ± 0.32e+13 1.02 ± 0.04e+15 1
MACS J0744.9+3927 116.21583 39.45917 0.6860 2 71260 7.87 ± 0.28 1.87 ± 0.06e+45 8.96 ± 0.19e+13 9.86 ± 0.30e+14 1
RX J0847.1+3449 131.79708 34.82111 0.5600 1 6908 7.11 ± 0.49e+44 0
MACS J0913.7+4056 138.40277 40.94315 0.4420 2 12430 5.39 ± 0.19 1.58 ± 0.06e+45 5.29 ± 0.09e+13 5.83 ± 0.20e+14 0
Abell 851 145.73601 46.98942 0.4069 213 40970 5.17 ± 0.16 6.13 ± 0.20e+44 5.04 ± 0.10e+13 5.53 ± 0.21e+14 1
MS 1054-03 164.25093 –3.62428 0.8231 326 25680 8.64 ± 0.66 1.49 ± 0.13e+45 1
UM 425 Cluster 170.83542 1.62944 0.7685 8 26090 14.5 ± 4.2 4.90 ± 0.34e+44 1.17 ± 0.06e+14 1.64 ± 0.06e+15 0
MS 1137.5+6624 175.09696 66.14485 0.7820 17 15560 7.43 ± 0.90 7.41 ± 1.05e+44 8.49 ± 0.58e+13 9.25 ± 0.59e+14 0
CLG J1205+4429 181.46410 44.48600 0.5915 10 25520 6.77 ± 3.32e+43 0
RXC J1206.2-0848 181.54991 –8.80001 0.4400 53 10200 9.36 ± 0.59 2.32 ± 0.08e+45 1.23 ± 0.05e+14 1.31 ± 0.05e+15 1
LCDCS 0504a 184.18845 –12.02147 0.7943 65 23460 5.49 ± 0.64 3.91 ± 0.50e+44 9.00 ± 0.93e+13 8.02 ± 0.77e+14 1
(184.18792) (–12.02139)
BMW-HRI J122657.3+333253 186.74167 33.54836 0.8900 35 65350 8.74 ± 0.42 2.02 ± 0.10e+45 1.16 ± 0.03e+14 1.21 ± 0.04e+15 –1
GHO 1322+3027 201.20091 30.19276 0.7550 38 36390 5.98 ± 1.33 8.91 ± 3.64e+43 5.17 ± 0.63e+13 6.11 ± 0.62e+14 0
ZwCl 1332.8+5043 203.58333 50.51506 0.6200 1 27860 5.08 ± 0.59 2.40 ± 0.51e+44 4.39 ± 0.33e+13 5.05 ± 0.42e+14 0
LCDCS 0829 206.88333 –11.76167 0.4510 50 32370 11.31 ± 0.24 7.75 ± 0.06e+45 1.58 ± 0.02e+14 1.69 ± 0.03e+15 1
LCDCS 0853 208.53958 –12.51639 0.7627 18 27420 3.65 ± 0.38e+44 0
RX J1354.2-0221 208.57042 –2.36306 0.5460 2 18390 2.18 ± 0.98 2.04 ± 0.62e+44 1.38 ± 0.29e+13 1.58 ± 0.29e+14 0
MACS J1423.8+2404b 215.95125 24.07972 0.5450 9 113400 5.3 ± 0.1 1.71 ± 0.05e+45 5.24 ± 0.10e+13 5.74 ± 0.10e+14 1 (Chandra)
GHO 1602+4312 241.10483 43.08131 0.8950 26 12000 8.96 ± 8.39e+43 0
MS 1621.5+2640 245.89863 26.56378 0.4260 104 2210 9.13 ± 3.46e+43 0
CXOU J205617.1-044155 314.07150 –4.69864 0.6002 1 16240 2.46 ± 1.02 1.98 ± 0.42e+44 5.02 ± 0.71e+13 3.59 ± 0.66e+14 0
MS 2053.7-0449 314.09321 –4.62873 0.5830 30 16240 4.81 ± 1.17 2.13 ± 0.56e+44 4.42 ± 0.63e+13 4.91 ± 0.62e+14 0
GHO 2143+0408 326.52000 4.38861 0.5310 1 20170 4.39 ± 0.43 1.51 ± 0.30e+44 4.60 ± 0.29e+13 4.77 ± 0.39e+14 0
RX J2202.7-1902 330.68708 –19.03611 0.4380 8 26060 4.97 ± 1.34 4.56 ± 2.07e+43 4.41 ± 0.57e+13 5.00 ± 0.58e+14 –1
RX J2328.8+1453 352.20792 14.88667 0.4970 1 25510 2.63 ± 0.53 4.28 ± 1.78e+43 2.03 ± 0.26e+13 2.20 ± 0.37e+14 0/–1

Notes. (1) Name given by NED (LCDCS clusters come from Gonzalez et al. 2001), (2) right ascension in degrees (J2000.0), (3) declination in degrees (J2000.0), (4) redshift, (5) number of galaxies with redshifts in the cluster range, (6) useful XMM-Newton exposure time (in seconds), (7) temperature of the X-ray gas, (8) X-ray luminosity in the [0.5, 8.0] keV band, (9) X-ray gas mass in the r500 radius, (10) total mass in the r500 radius, (11) subtructure inside the cluster (1 means yes, –1 means no, 0 means not detectable with data in hand).

(a)

The position given for LCDCS 504 comes from Guennou et al. (2013) where we determined the centre as the position of the cD, whereas the position given in parentheses was obtained from NED.

(b)

Cluster MACS J1423.8+2404 did not have any XMM-Newton public data, but we collected Chandra data with enough depth to be able to subtract a β-model and search for substructures.

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