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Table 3

Best-fit parameters for the morphology of HESS J1813–178B in different energy bands, for both Fermi-LAT (F1 – F6) and H.E.S.S. datasets (H1 large – H3 large).

Energy [GeV] RA [º] Dec [º] σM[º] e
F1 1.0–2.0 273.46 ± 0.02 −17.67 ± 0.02 0.39 ± 0.04 0.81 ± 0.05
F2 2.0–4.0 273.48 ± 0.03 −17.69 ± 0.03 0.42 ± 0.04 0.85 ± 0.04
F3 4.0–7.5 273.38 ± 0.04 −17.66 ± 0.06 0.39 ± 0.08 0.87 ± 0.07
F4 7.5–18 273.26 ± 0.09 −17.52 ± 0.12 0.53 ± 0.11 0.75 ± 0.19
F5 18–58 273.17 ± 0.10 −17.77 ± 0.08 0.57 ± 0.16 0.77 ± 0.21
F6 58–1.0 × 103 273.22 ± 0.20 −17.75 ± 0.13 0.71 ± 0.19 0.92 ± 0.08

H1 small (0.4–1.3) × 103 273.393 ± 0.005 −17.832 ± 0.005 0.054 ± 0.004
H2 small (1.3–5.7) × 103 273.397 ± 0.006 −17.834 ± 0.007 0.064 ± 0.005
H3 small (5.7–100) × 103 273.4O8 ± 0.009 −17.817 ± 0.009 0.035 ± 0.006

H1 large (0.4–1.3) × 103 273.61 ± 0.08 −17.48 ± 0.09 0.87 ± 0.12 0.88 ± 0.04
H2 large (1.3–5.7) × 103 273.41 ± 0.09 −17.42 ± 0.11 0.48 ± 0.09 0.48 ± 0.38
H3 large (5.7–100) × 103 273.65 ± 0.11 −17.18 ± 0.10 0.41 ± 0.09 0.00 ± 0.02

Notes. An elongated Gaussian model was assumed in all cases and the 1σ statistical uncertainties are given. Additionally, the best-fit values for the symmetrical Gaussian were used to account for the emission from HESS J1813–178A.

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