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Table 3.

Properties of cavities in our sample derived using the hybrid X-ray–radio method.

(a) (b) (c) (d) (e) (f) (g) (h) (i)
Cluster name Redshift Rl Rw R V p tbuoy Pcav
(kpc) (kpc) (kpc) (kpc3) (keV cm−3) (107 yr) (1042 erg s−1)
EGSXG J1420.5+5308 (N) 0.734 43.3 40.0 105 3 . 04 0.21 + 0.35 × 10 5 $ 3.04^{+0.35}_{-0.21} \times 10^5 $ 6 . 15 3.02 + 3.05 × 10 3 $ 6.15^{+3.05}_{-3.02} \times 10^{-3} $ 25 . 5 4.7 + 23.1 $ 25.5^{+23.1}_{-4.7} $ 42 . 9 28.4 + 27.3 $ 42.9^{+27.3}_{-28.4} $
EGSXG J1420.5+5308 (S) 0.734 51.7 35.7 112 3 . 03 0.29 + 1.14 × 10 5 $ 3.03^{+1.14}_{-0.29} \times 10^5 $ 5 . 77 2.96 + 2.99 × 10 3 $ 5.77^{+2.99}_{-2.96} \times 10^{-3} $ 25 . 2 4.2 + 17.9 $ 25.2^{+17.9}_{-4.2} $ 41 . 1 24.1 + 24.0 $ 41.1^{+24.0}_{-24.1} $
EGSXG J1416.2+5205 (N) 0.832 3.04 2.66 7.53 93 . 8 38.9 + 55.5 $ 93.8^{+55.5}_{-38.9} $ 1 . 86 0.75 + 1.20 × 10 2 $ 1.86^{+1.20}_{-0.75} \times 10^{-2} $ 1 . 36 0.56 + 1.38 $ 1.36^{+1.38}_{-0.56} $ 0 . 49 0.29 + 0.64 $ 0.49^{+0.64}_{-0.29} $
EGSXG J1416.2+5205 (S) 0.832 2.28 2.55 7.53 57 . 9 26.6 + 38.4 $ 57.9^{+38.4}_{-26.6} $ 1 . 87 0.75 + 1.20 × 10 2 $ 1.87^{+1.20}_{-0.75} \times 10^{-2} $ 2 . 19 0.65 + 1.42 $ 2.19^{+1.42}_{-0.65} $ 0 . 28 0.18 + 0.40 $ 0.28^{+0.40}_{-0.18} $
RX J1226+3333 (N) 0.890 5.47 2.64 6.21 195 82 + 132 $ 195^{+132}_{-82} $ 1 . 03 0.63 + 1.75 $ 1.03^{+1.75}_{-0.63} $ 1 . 06 0.24 + 0.49 $ 1.06^{+0.49}_{-0.24} $ 108 73 + 233 $ 108^{+233}_{-73} $
RX J1226+3333 (S) 0.890 5.32 1.79 6.21 89 . 4 50.1 + 84.7 $ 89.4^{+84.7}_{-50.1} $ 1 . 03 0.62 + 1.75 $ 1.03^{+1.75}_{-0.62} $ 1 . 07 0.33 0.67 $ 1.07^{0.67}_{-0.33} $ 46 . 7 34.8 + 114.6 $ 46.7^{+114.6}_{-34.8} $

Notes. Columns: (a) cluster name; (b) cluster redshift; (c) cavity radius along the jet axis; (d) cavity radius perpendicular to the jet axis; (e) central cavity distance from the AGN core; (f) cavity volume; (g) ICM pressure at the projected distance of the radio lobe to the AGN core; (h) buoyancy timescale; (i) cavity power.

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