Table 4
Fermi-LAT and H.E.S.S. combined fit results.
Name | ϕ0(E0) 10−12 cm−2 s−1 TeV−1 | α | β | E0 TeV | Epeak GeV |
---|---|---|---|---|---|
SHBL J001355.9-185406 | 2.24 ± 0.63 | 2.05 ± 0.14 | 0.04 ± 0.05 | 0.362 | <0.3 · 103 |
NGC 253 | 0.96 ± 0.06 | 2.38 ± 0.06 | 0.04 ± 0.02 | 0.426 | − |
1ES 0229+200 | 1.63 ± 0.03 | 1.76 ± 0.07 | 0.03 ± 0.04 | 0.607 | <5.11 · 103 |
PKS 0301-243 | 37. ± 3.3 | 2.43 ± 0.04 | 0.14 ± 0.01 | 0.213 | ![]() |
1ES 0414+009 | 7.8 ± 0.3 | 1.73 ± 0.08 | −0.04 ± 0.03 | 0.287 | − |
PKS 0447-439 | 40.6 ± 1.7 | 2.39 ± 0.02 | 0.14 ± 0.01 | 0.316 | 13 ± 1.0 |
PKS 0548-322 | 3.30 ± 0.15 | 2.08 ± 0.08 | 0.09 ± 0.04 | 0.373 | ![]() |
PKS 0625-354 | 8.23 ± 0.96 | 2.25 ± 0.07 | 0.10 ± 0.02 | 0.349 | ![]() |
1RXS J101015.9-311909 | 9.15 ± 0.42 | 2.30 ± 0.11 | 0.20 ± 0.05 | 0.281 | ![]() |
1ES 1101-232 | 16.1 ± 0.1 | 1.70 ± 0.04 | 0.034 ± 0.02 | 0.316 | <15.4 · 103 |
1ES 1312-423 | 5.94 ± 0.54 | 2.44 ± 0.17 | 0.37 ± 0.11 | 0.310 | ![]() |
PKS 1440-389 | 43.8 ± 1.0 | 2.36 ± 0.03 | 0.16 ± 0.01 | 0.259 | 18.6 ± 1.1 |
PKS 1510-089 | 20.0 ± 2.5 | 2.88 ± 0.05 | 0.11 ± 0.01 | 0.213 | − |
AP Lib | 10.2 ± 0.9 | 2.51 ± 0.04 | 0.09 ± 0.01 | 0.337 | ![]() |
1ES 2322-40.9 | 25.4 ± 2.1 | 2.12 ± 0.07 | 0.12 ± 0.03 | 0.235 | ![]() |
PKS 2005-489 | 17.4 ± 0.1 | 2.29 ± 0.02 | 0.13 ± 0.01 | 0.386 | ![]() |
PG 1553+113 | 63.7 ± 0.5 | 2.51 ± 0.02 | 0.24 ± 0.01 | 0.287 | ![]() |
RGB J0152+017 | 9.7 ± 1.8 | 2.17 ± 0.05 | 0.09 ± 0.02 | 0.287 | ![]() |
H 2356-309 | 15.3 ± 0.1 | 1.88 ± 0.02 | 0.08 ± 0.01 | 0.287 | ![]() |
1ES 0347-121 | 9.7 ± 1.8 | 2.17 ± 0.05 | 0.09 ± 0.02 | 0.287 | ![]() |
Notes. The first column gives the name of the source. Data were fitted with a log-parabola model, corrected for EBL absorption. The normalisation ϕ0(E0) and spectral parameters (α and β) are given. The fifth column gives the energy E0 at which the normalisation is evaluated. The last column presents the calculated peak energy Epeak or the corresponding upper limit at 99% CL in a SED representation. If no value is given, the peak or the upper limit cannot be computed (see text). Errors are statistical only.
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