Table 3
Resulting best-fit values for I0 and re, as well as the total flux density 
from integrating the spherical model with the best-fit values.
| Source name | I0 [μJy arcsec−2 ] | re [kpc] |  |
d |  |
 |
 |
 |
|---|---|---|---|---|---|---|---|---|
| PSZ2G147.88+53.24 |  |
 |
16.9 ± 2.0 | 2.5 | 16.4 ± 2.0 | 14.7 ± 1.6 | 16.0 ± 1.8 | 0.79 |
| PSZ2G147.88+53.24 (mask) |  |
 |
16.0 ± 2.0 | 2.2 | 14.0 ± 1.7 | 13.0 ± 1.4 | 15.5 ± 1.7 | 0.79 |
| PSZ2G149.22+54.18 |  |
 |
244.9 ± 29.7 | 2.5 | 236.8 ± 29.0 | 261.0 ± 30.6 | 271.3 ± 31.7 | 1.24 |
| PSZ2G084.69+42.28 |  |
 |
5.5 ± 1.6 | 1.9 | 4.3 ± 1.2 | 3.4 ± 0.5 | 4.7 ± 0.8 | 0.05 |
| MCXCJ1036.1+5713 |  |
 |
9.8 ± 1.1 | 3.6 | 11.7 ± 1.3 | 9.9 ± 1.1 | 8.6 ± 0.9 | 0.57 |
Notes. Parameter d denotes half of the largest linear size of the 3σ contours in e-folding radii, and
is the flux density obtained by integrating up to that value of d.
is the flux density measured within 3σ
(2σ for PSZ2G084.69+42.28) contours and 
is the flux density measured in a spherical region with a radius of 2.6re.
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