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Table 2.

Results of our analysis for all the clusters in our sample.

Cluster r500 T M500 σv Rccc Rqcf Rccc Rqcf Ref
(kpc) (keV) (1014 M) km s−1 (kpc) (kpc) (10−2r500) (10−2r500)
A2199 1087 (a)
A496 1218 ≤10.0 ≤0.8 (c)
2A0335 1042 (b)
A2589 997 ≤15 ≤15 ≤1.5 ≤1.5 (c)
MKW3S 896 ≤10 ≤10 ≤1.1 ≤1.1 (c)
Hydra 955 11.0 ≤1.2 (a)
A85 1124 (a)
A2626 875 ≤10 ≤20 ≤1.1 ≤2.3 (c)
A133 1014 (a)
SERSIC159 788 (a)
A1991 753 (a)
A3112 1060 (a)
A2029 1441 (c)
A2597 948 (a)
A3921 1134 ≤30 ≤30 ≤2.6 ≤2.6 (c)
A2244 1149 ≤10 ≤100 ≤0.9 ≤8.7 (c)
RXCJ1558.3 1088 ≤30.0 ≤2.8 (a)
PKS0745 1742 (a)
RXCJ1524.2 1058 (b)
RXCJ0352.9 825 (a)
A1664 877 (c)
A2204 1531 (c)
A907 1076 (c)
HerculesA 998 (c)
RXJ2014.8 1250 (a)
A1204 846 (a)
Zw2701 1020 ≤10.0 ≤1.0 (c)
RXCJ1504 1191 (c)
RXCJ1459.4 1031 (c)
4C+55.16 997 (c)
CL2089 881 (c)
RXJ2129.6 1148 (a)
A1835 1274 (c)
RXCJ1023.8 998 (c)
CL0348 799 (c)
MS1455.0 1014 (c)
ZW3146 1187 (c)

Notes. Column 1: Cluster name; Col. 2: Value of r500; Col. 3: Core-excised temperature (for r > 40 kpc and r < r500); Col. 4: Total mass within R500; Col. 5: Value of σv calculated from Eq. (9); Col. 6: Cool-core condensation radius defined by the condition tcool(Rccc)/teddy(Rccc) = 1 ; Col. 7: Quenched cooling flow radius defined by the condition tcool(Rqcf)/[25 tff(Rqcf)] = 1.; Cols. 8 and 9: Rccc and Rqcf in units of 10−2 × r500; Col. 10: Reference of σv measurements to each cluster, where (a) is Gaspari et al. (2018), (b) is Olivares et al. (2019), and (c) is this work using Eq. (9).

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