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Table 2:

Radio properties of the mini halos derived from the fit procedure.
Cluster FWHM re re $I_{0_{\rm MH}}$ $S_{\rm MH}$ $I_{0_{\rm PS}}$ $FWHM_{\rm PS}$ $S_{\rm PS}$ $\langle J\rangle$ $\chi^2_{\rm RED}$
  arcsec arcsec kpc $\mu $Jy/arcsec2 mJy $\mu $Jy/arcsec2 arcsec mJy erg s-1 Hz-1 cm-3  

A1835
53 $26^{\rm +18}_{-8}$ $102^{\rm +70}_{-31}$ $1.78^{\rm +4.95}_{-1.32}$ $6.0^{\rm +0.8}_{-0.7}$ $8.68^{\rm +0.65}_{-1.11}$ $57^{\rm +2}_{-3}$ $32.2^{\rm +0.8}_{-0.7}$ $3.3^{\rm +2.2}_{-1.3}\times 10^{-42}$ 0.03

A2029
53 $37^{\rm +4}_{-4}$ $53^{\rm +6}_{-6}$ $2.75^{\rm +0.92}_{-0.64}$ $18.8^{\rm +1.3}_{-1.1}$ $129^{\rm +7}_{-7}$ $57^{\rm +1}_{-1}$ $480.0^{\rm +19.5}_{-19.4}$ $5.4^{\rm +1.9}_{-1.3}\times 10^{-42}$ 0.5

OPHIUCHUS
92 $191^{\rm +23}_{-19}$ $105^{\rm +13}_{-11}$ $0.58^{\rm +0.08}_{-0.07}$ $106.4^{\rm +10.4}_{-8.9}$ $2.47^{\rm +0.22}_{-0.21}$ $102^{\rm +6}_{-5}$ $29.0^{\rm +2.0}_{-2.0}$ $4.7^{\rm +0.9}_{-0.8}\times 10^{-43}$ 2.9
Column 2: FWHM of the circular Gaussian beam; Col. 6: mini-halo radio flux density calculated up to 3re; Col. 10: average radio emissivity over the volume of a sphere of radius 3re, k-corrected with $\alpha =1$.

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