Table 4.
Properties of the sources with chances of observation as reported in Table 3.
| Source | RA, DEC | Redshift | νFν, 2 − 10 keV | νFν, 100 GeV, LP model | νFν, 100 GeV, BPL model |
|---|---|---|---|---|---|
| [10−12 erg s−1 cm−2] | [10−12 erg s−1 cm−2] | [10−12 erg s−1 cm−2] | |||
| 5BZBJ1253+3826 | 12:53:00.90, +38:26:26.01 | 0.371 | ![]() |
0.17 – 0.63 | 0.13 – 0.15 |
| 5BZBJ1636−1248 | 16:36:58.42, −12:48:36.5 | 0.246 | ![]() |
0.30 – 1.52 | 0.21 – 0.51 |
| 5BZBJ1251−2958 | 12:51:34.88, −29:58:42.88 | 0.382 | ![]() |
0.37 – 1.46 | 0.29 – 0.64 |
| 5BZBJ0040−2719 | 00:40:16.40, −27:19:11.60 | 0.172 | ![]() |
0.19 – 1.00 | 0.12 – 0.18 |
| 5BZBJ1057+2303 | 10:57:23.09, +23:03:18.79 | 0.379 | ![]() |
0.51 –1.38 | 0.58 – 1.16 |
| 5BZBJ1258+0134 | 12:58:54.59, +01:34:41.41 | -99 | ![]() |
0.16 – 1.10 | 0.09 – 0.37 |
Notes. The coordinates (RA, DEC) and redshift are reported from the 5BZCAT catalogue, while the fluxes come from this work. The X-ray flux in the band 2–10 keV comes from the X-ray analysis results, while the VHE flux at 100 GeV corresponds to the range of fluxes established by the models in Sect. 5. As mentioned in the text, we caution that the lack of a spectroscopic redshift can affect the reliability of the VHE predictions for 5BZBJ1258+0134.
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