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Table 2

Best-fit results for the SED fitting of the LHAASO spectrum and the XMM-Newton upper limits on the diffuse emission when fixing the spectral index p.

p Ecut (TeV) Ecut (TeV) We (erg) Max log(L) BIC
1.2 15620+15$156^{+15}_{-20}$ 33 ± 2 1.87 · 1044 –3.46 11.53
1.4 16418+14$164^{+14}_{-18}$ 352+1$35^{+1}_{-2}$ 2.29 · 1044 –3.29 11.19
1.6 1639+28$163^{+28}_{-9}$ 35.10.8+3.6$35.1^{+3.6}_{-0.8}$ 3.29 · 1044 –3.09 10.78
1.8 19619+26$196^{+26}_{-19}$ 459+3$45^{+3}_{-9}$ 4.75 · 1044 –2.93 10.46
2.0 19929+26$199^{+26}_{-29}$ 464+3$46^{+3}_{-4}$ 1.20 · 1045 –2.78 10.16
2.2 23138+30$231^{+30}_{-38}$ 555+4$55^{+4}_{-5}$ 4.16 · 1045 –2.68 9.96
2.4 24724+39$247^{+39}_{-24}$ 603+5$60^{+5}_{-3}$ 2.24 · 1046 –2.65 9.90

Notes. In addition to the best-fit values for the cut-off energy Ecut, its correspondent photon energy Ecut,γ and the total energy content We, we report the values of the maximum logarithmic likelihood and of the Bayesian information criterion (BIC) obtained with the naima fitting process.

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