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Table 5.

Summary of the comparison between different models for the flaring epoch MJD 54761.

Reference Agudo et al. (2011)(b) Ackermann (2012)(c) Baring et al. (2017)(d)
Model components (a) Synch + SSC (dom.) Synch + EC (DT) (dom.) + SSC + BC Synch + EC (BC) (dom.) + SSC
Bulk Lorentz factor Γ 39.4 20 (Γb = 10) 35
Viewing angle Θ ≦2.4° 2.3° 1.7°
Doppler factor δ 24 20 (δb = 16)
Opening angle θ 2.3° 2.9° (θb = 2.3°)
Location r 12 pc 1.7 pc
Size of the emission region R 1 × 1016 cm
Magnetic field intensity B 0.22 G 2.5 G
Electrons γmin 100
γmax 5.8 × 103 1.61 × 103
ne(E) doubly broken pwl. See footnote (e)
p1 = 1.5, p2 = 2.03, p3 = 3.9
Protons ne/np+ 9
Disk luminosity Ldisk 4 × 1045 erg s−1 3.4 × 1044 erg s−1
Disk temperature Tdisk 3.5 × 103 K (f) 1 × 103 K
Disk radius Rdisk 6 × 1017 cm

Notes.

(a)

The components considered are synchrotron (Synch), synchrotron self-Compton (SSC), external Compton (EC) from the dusty torus (DT), and bulk-Compton (BC).

(b)

The values for Agudo et al. (2011) do not come from a SED model, but from the DCF analysis and kinematic parameters from VLBI images, assuming a SSC scenario. The value for Γ is not cited in the paper, it is the one obtained by Weaver et al. (2022) for the same component in VLBI.

(c)

Parameters for the blazar zone (their model includes a second population of relatvistic cold electrons to account for the secondary soft X-ray bump, whose parameters are indicated between parenthesis.

(d)

The secondary soft x-ray bump is modeled by bulk Comptonization of a background seed field from a dusty torus); the H.E. bump by the external Compton of the electron population.

(e)

The energy distribution is simulated from diffusive shock acceleration (DSA) and the resulting parameters are not explicitly indicated.

(f)

From the given radiation temperature of 0.3 eV.

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