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Table B.1.

Mass accretion rates for all Kerr and dilaton model configurations.

Metric/Accr. eDF Rhigh
1 10 20 40
thermal 0.190 ± 0.024 6.10 ± 0.80 14.4 ± 1.8 20.9 ± 2.6
Kerr SANE ε = 0 0.190 ± 0.024 6.1 ± 0.8 14.6 ± 1.8 21.3 ± 2.7
ε = 0.015 0.190 ± 0.024 6.1 ± 0.8 14.6 ± 1.8 21.2 ± 2.6

thermal 0.211 ± 0.028 9.0 ± 1.2 26.0 ± 4.0 41.0 ± 6.0
Dilaton SANE ε = 0 0.211 ± 0.028 9.1 ± 1.2 26.9 ± 4.0 43.3 ± 6.0
ε = 0.015 0.211 ± 0.028 9.1 ± 1.2 26.8 ± 4.0 43.1 ± 6.0

thermal 0.124 ± 0.019 1.27 ± 0.20 1.68 ± 0.27 0.90 ± 0.14
Kerr MAD ε = 0 0.124 ± 0.020 1.29 ± 0.21 1.71 ± 0.27 0.90 ± 0.15
ε = 0.015 0.124 ± 0.020 1.29 ± 0.20 1.70 ± 0.27 0.90 ± 0.14

thermal 0.127 ± 0.018 0.82 ± 0.12 1.06 ± 0.15 1.30 ± 0.18
Dilaton MAD ε = 0 0.127 ± 0.018 0.85 ± 0.12 1.13 ± 0.16 1.40 ± 0.20
ε = 0.015 0.127 ± 0.018 0.85 ± 0.12 1.12 ± 0.16 1.39 ± 0.20

Notes. Thermal, kappa with ε = 0 and kappa with ε = 0.015 model mass acretion rates, in units of 10−8 M/yr (Kerr a = 0.6, Dilaton b = 0.504). obtained by multiplying the BHOSS accretion parameter by the respective GRMHD accretion rates reported in Table 3. All obtained to fit the 230 GHz flux to 2.5 Jy between 11 000 M and 12 000 M.

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