Table A.1
Best-fitting X-ray pressure profile parameters.
| Cluster | R 500 | P 500 | P 0 | c 500 | α | γ | χ 2 | d.o.f. |
| (Mpc) | (10-3keV cm-3) | |||||||
|
|
||||||||
| A68 | 1.030 | 2.828 | 24.01 | 1.54 | 1.31 | 0.000 | 1.8 | 7 |
| A209 | 1.344 | 4.328 | 14.51 | 0.78 | 0.79 | 0.008 | 0.9 | 13 |
| A267 | 0.964 | 2.345 | 26.66 | 1.18 | 0.89 | 0.000 | 6.3 | 8 |
| A291 | 1.044 | 2.558 | 1.58 | 1.41 | 1.82 | 0.919 | 0.5 | 9 |
| A383 | 0.989 | 2.256 | 14.61 | 1.49 | 0.97 | 0.422 | 2.4 | 7 |
| A521 | 1.015 | 2.699 | 1.75 | 1.17 | 3.53 | 0.434 | 1.7 | 6 |
| A520 | 1.056 | 2.654 | 9.67 | 1.29 | 1.88 | 0.000 | 7.7 | 6 |
| A963 | 1.055 | 2.667 | 8.81 | 0.98 | 0.97 | 0.463 | 1.0 | 9 |
| A1835 | 1.363 | 4.934 | 5.36 | 1.81 | 1.71 | 0.721 | 8.5 | 8 |
| A1914 | 1.115 | 2.769 | 72.97 | 1.56 | 0.95 | 0.000 | 30.1 | 6 |
| ZwCl1454.8+2233 | 0.914 | 2.242 | 706.26 | 0.71 | 0.44 | 0.000 | 14.3 | 6 |
| ZwCl1459.4+4240 | 0.998 | 2.870 | 18.52 | 1.20 | 1.10 | 0.000 | 5.3 | 7 |
| A2034 | 1.174 | 2.726 | 9.73 | 1.78 | 1.72 | 0.000 | 10.0 | 8 |
| A2219 | 1.302 | 4.258 | 21.92 | 1.03 | 0.99 | 0.056 | 4.5 | 9 |
| RXJ1720.1+2638 | 1.034 | 2.344 | 79.14 | 0.71 | 0.58 | 0.178 | 10.9 | 8 |
| A2261 | 1.305 | 4.244 | 87.01 | 1.54 | 0.70 | 0.000 | 0.1 | 0 |
| RXJ2129.6+0005 | 1.079 | 2.967 | 6.24 | 1.23 | 1.20 | 0.612 | 1.4 | 9 |
| A2390 | 1.244 | 3.913 | 7.81 | 0.91 | 1.13 | 0.467 | 3.1 | 8 |
| A2631 | 1.078 | 3.260 | 7.44 | 1.24 | 1.61 | 0.200 | 0.0 | 6 |
Notes. Column (2): R500, the radius corresponding to a density contrast of 500, estimated from the weak lensing mass analysis of Okabe & Umetsu (2008); Okabe et al. (2010). Column (3): P500 as defined by Eq. (5) of Arnaud et al. (2010). Columns (4) to (7) give the best-fitting GNFW parameters for the pressure profiles (Eq. (2)). The external slope parameter β has been fixed to 5.49 (see text). No uncertainties are given as the GNFW parameters are highly degenerate. The profiles and best-fitting GNFW models are illustrated in Fig. A.1.
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