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Table 1.

Parameters of the non-thermal pressure model for the X-COP clusters.

Cluster α500/α200 (E19) F500/F200 γ P0NT/P0T β α500/α200 (this work)
A1644 1.023 ± 0.095/1.063 ± 0.108 1.117 ± 0.066
A1795 0.942 ± 0.073/0.931 ± 0.058 1.090 ± 0.096 1.79e−02 0.937
A2029 0.929 ± 0.072/0.882 ± 0.058 1.249 ± 0.068 1.51e−03 0.749
A2142 0.829 ± 0.063/0.798 ± 0.050 1.252 ± 0.060 3.80e−02 1.038
A2255 0.856 ± 0.085/0.918 ± 0.123 1.173 ± 0.040 4.68e+00 1.597
A2319 0.693 ± 0.056/0.565 ± 0.041 1.304 ± 0.043 1.20e−03 0.484
A3158 0.903 ± 0.076/0.865 ± 0.072 1.194 ± 0.055 6.59e−03 0.838
A3266 0.992 ± 0.096/1.241 ± 0.217 0.899 ± 0.031
A644 0.992 ± 0.113/0.964 ± 0.116 1.356 ± 0.118
A85 0.873 ± 0.067/0.843 ± 0.058 0.871 ± 0.045 5.20e−02 0.735
RXC1825 0.985 ± 0.077/0.865 ± 0.060 0.984 ± 0.050
ZW1215 1.236 ± 0.126/1.457 ± 0.162 0.999 ± 0.053

Notes. For each object, we quote: the constraints on α at R500 and R200 both in Eckert et al. (2019) (second column) and in the present work (last column); the estimated Fi; the effective polytropic index, γ, measured in the radial range [0.3, 1.6]R500; the parameters 1/p0 = P0NT/P0T and β, from which α is estimated (see Eq. (8)). The quoted errors are at 1σ c.l., and the quoted errors on α are obtained from 100 Monte Carlo runs by propagating the statistical errors on the observed gas density and pressure profiles, and the observed gas fractions.

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