Table 2
Flux density measurements from MSSS, TGSS, and higher frequencies from literature used for the spectral fitting discussed in Sect. 3.5.
Source | MSSS 140 MHz | TGSS 148 MHz | P-band | 750 MHz | L-band | S-band | C-band | |||||
S ν | S ν | ν | S ν | ν | S ν | ν | S ν | ν | S ν | ν | S ν | |
(Jy) | (Jy) | (MHz) | (Jy) | (MHz) | (Jy) | (MHz) | (Jy) | (MHz) | (Jy) | (MHz) | (Jy) | |
|
||||||||||||
A2199 | 54.3 ± 6.1 | 52.9 ± 5.6 | 324 | 24.00 ± 0.96 | 7501 | 9.1900 ± 0.0049 | 14002 | 3.68 ± 0.12 | 27003 | 1.21 ± 0.06 | 4675 | 0.313 ± 0.012 |
MS 0735.6+7421 | 5.30 ± 0.83 | 3.95 ± 0.46 | 330 | 0.80 ± 0.03 | 1425 | 0.021 ± 0.001 | ||||||
2A 0335+096 | 1.10 ± 0.21 | 1.05 ± 0.19 | 324 | 0.21 ± 0.01 | 14902 | 0.0367 ± 0.0018 | 4860 | 0.01 ± 0.001 | ||||
Perseus | 58.8 ± 6.3 | 42.4 ± 4.4 | 4084 | 29.00 ± 0.04 | 7501 | 21.82 ± 0.28 | ||||||
A262 | 0.57 ± 0.15 | 0.540 ± 0.091 | 324 | 0.299 ± 0.012 | 1365 | 0.0734 ± 0.0030 | ||||||
MKW3s | 17.3 ± 2.2 | 15.6 ± 1.8 | 327 | 4.73 ± 0.18 | 1440 | 0.0897 ± 0.0040 | 4860 | 0.0025 ± 0.0001 | ||||
A2052 | 58.5 ± 6.7 | 59.4 ± 6.3 | 330 | 30.9 ± 1.2 | 7501 | 11.76 ± 0.041 | 1490 | 5.7 ± 0.2 | 27005 | 2.02 ± 0.04 | 4860 | 0.72 ± 0.03 |
A478 | 0.53 ± 0.14* | 0.305 ± 0.050 | 327 | 0.11 ± 0.01 | 1440 | 0.027 ± 0.001 | ||||||
Zw 3146 | 0.259 ± 0.056** | 0.0174 ± 0.0056 | 324 | 0.016 ± 0.004*** | 4860 | 0.00139 ± 0.00007 | ||||||
Zw 2701 | 1.36 ± 0.18 | 1.35 ± 0.15 | 324 | 0.21 ± 0.01 | 4860 | 0.0043 ± 0.0002 | ||||||
A1795 | 7.47 ± 0.90 | 6.08 ± 0.67 | 327 | 3.36 ± 0.14 | 1465 | 0.88 ± 0.04 | 27003 | 0.48 ± 0.03 | 48506 | 0.261 ± 0.034 | ||
RBS 797 | 0.133 ± 0.035 | 0.174 ± 0.033 | 324 | 0.104 ± 0.006 | 1475 | 0.021 ± 0.001 | 4860 | 0.0042 ± 0.0003 | ||||
MACS J1423.8 | 0.103 ± 0.044 | 0.054 ± 0.013 | 327 | 0.0269 ± 0.002 | 1425 | 0.0044 ± 0.0002 | ||||||
A1835 | 0.150 ± 0.055 | 0.107 ± 0.021 | 327 | 0.095 ± 0.007 | 1400 | 0.031 ± 0.001 | 4760 | 0.0099 ± 0.0004 | ||||
M84 | 14.9 ± 1.9 | 324 | 11.1 ± 0.5 | 1425 | 05.6 ± 0.2 | 4860 | 2.28 ± 0.09 | |||||
M87 | 436 ± 45 | 324 | 124 ± 5 | 1400 | 138 ± 6 | 4860 | 59 ± 2 | |||||
A133 | 9.6 ± 1.0 | 330 | 3.60 ± 0.10 | 1425 | 0.132 ± 0.005 | |||||||
Hydra A | 317 ± 36 | 333 | 152 ± 6 | 7507 | 79.9 ± 3.2 | 1423 | 39.2 ± 1.6 | 27008 | 23.50 ± 0.93 | 4760 | 15.0 ± 0.6 | |
Centaurus | 19.5 ± 2.0 | 327 | 12.3 ± 0.5 | 6257 | 7.160 ± 0.040 | 1565 | 3.4 ± 0.1 | 27009 | 2.458 ± 0.048 | 4760 | 1.37 ± 0.06 | |
HCG 62 | 0.0090 ± 0.0039 | 324 | 0.008 ± 0.002 | 1440 | 0.0050 ± 0.0004 | |||||||
Sersic 159/03 | 4.23 ± 0.45 | 324 | 1.53 ± 0.06 | 1425 | 0.22 ± 0.01 | 4860 | 0.056 ± 0.002 | |||||
A2597 | 14.7 ± 1.5 | 328 | 8.3 ± 0.3 | 1400 | 1.86 ± 0.07 | 4985 | 0.37 ± 0.02 | |||||
A4059 | 22.8 ± 2.4 | 328 | 9.93 ± 0.40 | 14402 | 1.285 ± 0.043 | 270010 | 0.35 ± 0.07 | 486011 | 0.12 ± 0.04 |
Notes. The values for MSSS, and TGSS derive from our analysis. The unreferenced values at higher frequencies come from Bîrzan et al. (2008). The numbers in superscripts reference the high frequency flux density measurements coming from the literature.
A478 is not resolved in the MSSS map and is blended with neighboring cluster members. Thus, the flux measurement at 140 MHz includes serious contributions from several surrounding sources.
Zw3146 is not resolved in the MSSS map and is blended with neighboring sources. Thus, the flux measurement at 140 MHz includes serious contributions from several surrounding sources.
Value not identical with the one cited in Bîrzan et al. (2008). We used the P-band map from Bîrzan et al. (2008) to measure the flux ourselves.
Reference. (1) Pauliny-Toth et al. (1966); (2) Condon et al. (1998); (3) Andernach et al. (1981); (4) Burbidge & Crowne (1979); (5) Wall & Peacock (1985); (6) Gregory & Condon (1991); (7) Haynes et al. (1975); (8) Wright & Otrupcek (1990); (9) Sadler (1984); (10) Vollmer et al. (2005); (11) Wright et al. (1994).
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