Open Access

Table C.2.

Best-fit values of the elliptical exponential model for each radio halo considered.

Name PRH (1024 W Hz−1) I0 (μJy arcsec−2) r1 (kpc) r2 (kpc) S/N χ2
PSZ2G008.31-64.74 7.06 ± 0.48 0.23 ± 0.01 1003 ± 59 376 ± 25 30.4 0.96
PSZ2G008.94-81.22 16.35 ± 1.06 2.80 ± 0.09 293 ± 12 246 ± 10 41.8 0.54
PSZ2G056.93-55.08 10.24 ± 0.65 0.83 ± 0.02 364 ± 23 270 ± 21 51.0 1.53
PSZ2G159.91-73.50 1.96 ± 0.35 0.55 ± 0.30 306 ± 115 205 ± 58 6.0 2.09
PSZ2G172.98-53.55 2.63 ± 0.21 0.46 ± 0.04 278 ± 46 204 ± 44 19.0 0.59
PSZ2G205.93-39.46 11.02 ± 0.95 1.67 ± 0.15 310 ± 29 172 ± 19 16.1 0.53
PSZ2G208.80-30.67 1.97 ± 0.68 0.38 ± 1.45 349 ± 249 226 ± 145 3.0 2.13
PSZ2G225.93-19.99 12.98 ± 0.78 2.30 ± 0.02 264 ± 10 177 ± 10 148.2 3.07
PSZ2G239.27-26.01 7.83 ± 0.48 1.33 ± 0.02 273 ± 11 181 ± 10 108.0 1.32
PSZ2G243.15-73.84 3.87 ± 0.25 0.57 ± 0.02 315 ± 20 193 ± 11 41.1 3.81
PSZ2G259.98-63.43 9.49 ± 0.65 6.12 ± 0.30 158 ± 9 131 ± 9 30.9 0.59
PSZ2G262.27-35.38 5.28 ± 0.35 0.27 ± 0.01 731 ± 37 340 ± 22 37.1 1.01
PSZ2G263.68-22.55 9.66 ± 0.72 1.30 ± 0.07 598 ± 43 251 ± 14 22.5 0.70
PSZ2G266.04-21.25 25.46 ± 1.60 5.72 ± 0.15 304 ± 11 187 ± 8 52.0 0.84
PSZ2G277.76-51.74 6.25 ± 0.44 0.28 ± 0.02 440 ± 31 409 ± 33 27.2 0.94
PSZ2G278.58+39.16 13.55 ± 0.82 4.74 ± 0.04 200 ± 10 177 ± 10 183.0 2.80
PSZ2G286.98+32.90 28.35 ± 1.71 2.36 ± 0.02 389 ± 7 293 ± 7 177.8 1.57
PSZ2G313.33+61.13 2.21 ± 0.13 1.40 ± 0.02 204 ± 10 146 ± 10 102.3 0.83
PSZ2G313.88-17.11 2.95 ± 0.28 1.54 ± 0.12 265 ± 31 153 ± 16 13.8 0.28
PSZ2G346.61+35.06 3.37 ± 0.21 0.34 ± 0.01 419 ± 12 393 ± 13 61.0 0.90
PSZ2G349.46-59.95 3.81 ± 0.27 1.44 ± 0.08 190 ± 12 151 ± 11 27.0 0.48

References. (1) cluster name; (2) total radio halo power at 1.28 GHz; (3) radio halo central surface brightness; (4-5) e-folding radii; (6) signal-to-noise ratio of the emission; (7) reduced chi-square of the fit.

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