Table 1.
Flux density and spectral indeces of our sample of radio halos
Cluster name |
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α1re | α3σ | Image |
---|---|---|---|---|---|---|---|
[mJy] | [mJy] | [mJy] | [mJy] | ||||
PSZ2G086.93+53.18 | 6 ± 3 | 25 ± 7 | 0.7 ± 0.2 | 3.1 ± 0.5 | −2.20 ± 0.61 | −2.15 ± 0.32 | T90 (=150 kpc) |
PSZ2G096.83+52.49 | 122 ± 21 | 288 ± 43 | 20.8 ± 2.2 | 43.8 ± 4.5 | −1.80 ± 0.30 | −1.92 ± 0.17 | T100 kpc |
PSZ2G099.86+58.45 | 34 ± 5 | 22 ± 4 | 6.5 ± 0.8 | 4.3 ± 0.6 | −1.67 ± 0.26 | −1.66 ± 0.27 | T50 kpc |
PSZ2G107.10+65.32N | 205 ± 14 | 1084 ± 69 | 65.5 ± 6.6 | 314.8 ± 31.5 | −1.16 ± 0.24 | −1.26 ± 0.04 | T100 kpc |
PSZ2G107.10+65.32S | 78 ± 15 | 248 ± 33 | 24.8 ± 2.9 | 83.7 ± 8.9 | −1.17 ± 0.46 | −1.11 ± 0.26 | T50 kpc |
PSZ2G111.75+70.37 | 37 ± 7 | 205 ± 26 | 5.1 ± 0.6 | 27 ± 3.0 | −2.02 ± 0.27 | −2.07 ± 0.14 | T100 kpc |
PSZ2G114.31+64.89 | 149 ± 12 | 324 ± 23 | 23.9 ± 2.4 | 43.2 ± 4.4 | −1.87 ± 0.16 | −2.05 ± 0.05 | T50 kpc |
PSZ2G133.60+69.04 | 318 ± 33 | 590 ± 54 | 62.7 ± 6.3 | 115.8 ± 12.1 | −1.66 ± 0.20 | −1.66 ± 0.11 | T50 kpc |
PSZ2G135.17+65.43 | 36 ± 8 | 50 ± 10 | 10.7 ± 1.2 | 16.6 ± 1.8 | −1.24 ± 0.47 | −1.12 ± 0.39 | T50 kpc |
PSZ2G139.18+56.37 | 303 ± 20 | 1249 ± 82 | 96.5 ± 9.7 | 292.3 ± 29.3 | −1.17 ± 0.24 | −1.48 ± 0.04 | T50 kpc |
PSZ2G143.26+65.24 | 33 ± 6 | 115 ± 14 | 7.3 ± 1.0 | 28.3 ± 3.0 | −1.54 ± 0.35 | −1.43 ± 0.19 | T100 kpc |
Notes. The table lists, from first to last column: cluster name, 54 MHz halo flux density estimated within 1 e-folding radius and within 3σ 144 MHz contours, 144 MHz halo flux density estimated within 1 e-folding radius and within 3σ 144 MHz contours, spectral index estimated within 1 e-folding radius and within 3σ 144 MHz contours, source-subtracted image used for flux density measurement (T50 kpc = taper 50 kpc, T100 kpc = taper 100 kpc, T90 = taper 90″).
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