Table 5
Comparison of the high-energy extrapolation from the 2LAC with H.E.S.S. upper limits.
| Object | z | E th | I(>Eth) | I2LAC(> Eth) |
Eth)
|
| [TeV] | [% C.U.] | [% C.U.] | [% C.U.] | ||
|
|
|||||
| 2FGL J1351.4+1115 | 0.40 | 0.48 | 0.7 | 40 | 0.2 |
| 1FGL J0022.2-1850 | 0.77−1.38 | 0.24 | 0.4 | 24 | 0.1 |
| 1FGL J0051.4-6242 | <1.12 | 0.58 | 0.9 | 37 | 0.5 |
| BZB J0543-5532 | 0.27 | 0.39 | 0.9 | 25 | 1.4 |
| 1FGL J0506.9-5435 | <1.07 | 0.95 | 2.3 | 65 | 0.2 |
| RBS 334 | 0.41 | 0.35 | 1.3 | 13 | 0.2 |
| PKS 0048-097 | 0.64 | 0.26 | 0.5 | 3.6 | 0.05 |
| 2FGL J0334.3-3728 | <1.34 | 0.26 | 0.9 | 7.3 | 1.0 |
| RBS 1049 | 0.25 | 0.39 | 1.2 | 5.0 | 0.4 |
| PMN J2345-1555 | 0.62 | 0.22 | 0.7 | 2.7 | 0.1 |
| RBS 421 | 0.29 | 0.29 | 0.6 | 1.8 | 0.2 |
| RBS 1752 | 0.45 | 0.29 | 0.3 | 1.0 | 0.04 |
Notes. Only objects with constraining limits are selected. I2LAC(>Eth) and Eth) are the 2LAC measurements extrapolated above Eth, taking into account the EBL absorption for the second quantity. When only an upper limit on the redshift is available, a value of z = 0.3 is assumed to derive these extrapolations. For 1FGL J0022.2-1850, the lower limit z > 0.77 is used.
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