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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 5.10.5+0.6$\[5.1_{-0.5}^{+0.6}\]$
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 13080+50$\[130_{-80}^{+50}\]$
PKS 0625-354 8.23 ± 0.96 2.25 ± 0.07 0.10 ± 0.02 0.349 185+4$\[18_{-5}^{+4}\]$
1RXS J101015.9-311909 9.15 ± 0.42 2.30 ± 0.11 0.20 ± 0.05 0.281 508+9$\[50_{-8}^{+9}\]$
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 7813+16$\[78_{-13}^{+16}\]$
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 0.360.11+0.17$\[0.36_{-0.11}^{+0.17}\]$
1ES 2322-40.9 25.4 ± 2.1 2.12 ± 0.07 0.12 ± 0.03 0.235 7423+33$\[74_{-23}^{+33}\]$
PKS 2005-489 17.4 ± 0.1 2.29 ± 0.02 0.13 ± 0.01 0.386 32.00.1+0.1$\[32.0_{-0.1}^{+0.1}\]$
PG 1553+113 63.7 ± 0.5 2.51 ± 0.02 0.24 ± 0.01 0.287 36.10.1+0.1$\[36.1_{-0.1}^{+0.1}\]$
RGB J0152+017 9.7 ± 1.8 2.17 ± 0.05 0.09 ± 0.02 0.287 38.70.1+0.2$\[38.7_{-0.1}^{+0.2}\]$
H 2356-309 15.3 ± 0.1 1.88 ± 0.02 0.08 ± 0.01 0.287 1.60.7+1.3$\[1.6_{-0.7}^{+1.3}\]$ · 103
1ES 0347-121 9.7 ± 1.8 2.17 ± 0.05 0.09 ± 0.02 0.287 38.70.1+0.2$\[38.7_{-0.1}^{+0.2}\]$

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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