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Table 1.

General properties of the clusters investigated in this study.

ID RA Dec z M200 R200 σ References
(hh:mm:ss) (dd:mm:ss) (1014M) (Mpc) (km s−1)
Abell 901/902
A901a 09:56:27 −09:57:22 0.16 1.3  ±  0.3 0.8  ±  0.1 880  ±  30
A901b 09:55:57 −09:59:03 0.16 1.3  ±  0.3 0.8  ±  0.1 940  ±  20 Heymans et al. (2008)
A902 09:56:34 −10:10:00 0.17 0.4  ±  0.2 0.6  ±  0.1 810  ±  20 Weinzirl et al. (2017)
SW Group 09:55:39 −10:10:19 0.17 0.6  ±  0.2 0.6  ±  0.1 590  ±  40

RXJ 1347
RXJ 1347-1145 13:47:31 −11:45:10 0.45 11.6  ±  3.0 1.9  ±  0.2 1160  ±  100 Lu et al. (2010)
RXJ 1347-1145 13:46:27 −11:54:28 0.47 5.6  ±  1.6 1.2  ±  0.2 780  ±  100

CL1604
CL1604+4304 16:04:22 43:04:56 0.90 3.3  ±  1.5 0.9  ±  0.2 720  ±  130 Lemaux et al. (2012),
CL1604+4321 16:04:34 43:21:14 0.92 1.8  ±  1.6 0.8  ±  0.1 690  ±  90 Wu et al. (2014)

XMMU J2235.3-2557 22:35:21 25:57:40 1.39 7.3  ±  1.3 1.1  ±  0.1 1180  ±  90 Jee et al. (2009)

HSC-CL2329 23:30:05 00:12:36 1.47 (a) < 400 Böhm et al. (2020)

HSC-CL2330 23:30:22 −00:24:00 1.47 (a) < 400 Böhm et al. (2020)

Notes. The table lists: IDs, right ascension, declination, redshift, virial mass (M200) and size (R200), velocity dispersion, and references for these measurements.

(a)

These two protoclusters are most probably not yet virialized structures. Thus, no velocity dispersion-based mass can be computed. See Böhm et al. (2020) for more details.

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