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Fig. 3.

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P1.4 GHz−M500 correlation plot of radio haloes. To account for the discrepancies between the ACT and Planck mass derivations, we use the uncorrected M500c values for the ACT clusters (Hilton et al. 2021). The solid line shows the best-fit relation, with parameters extracted from the low-redshift sample (z ∼ 0.2) presented in Cassano et al. (2013), this fit was performed using linear regression in the log-log space by adopting the BCES-bisector method. The Di Gennaro et al. (2021a) sample consists of radio haloes at z > 0.6, and the Knowles et al. (2021) sample covers 0.22 < z < 0.65. We also include El Gordo, which is at z = 0.87 (Lindner et al. 2014).

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