Table 4.
Parameters for the models shown in Figs. 1, 2, 3, 4, and 6.
Source | z | ![]() |
Ld | LT/Ld | Rdiss | RBLR | RT | P′inj |
---|---|---|---|---|---|---|---|---|
M⊙ | 1045 erg s−1 | 1015 cm | 1015 cm | 1015 cm | 1045 erg s−1 | |||
PKS 0123+25 | 2.358 | 1.5e9 | 58.5 | 0.3 | 270 | 764 | 3.1e4 | 0.017 |
PKS 0123+25 no torus | 2.358 | 1.5e9 | 58.5 | 0 | 225 | 764 | – | 0.012 |
PKS 0123+25 no torus | 2.358 | 1.5e9 | 58.5 | 0 | 3.6e3 | 764 | – | 0.3 |
PKS 0123+25 (ψ = 1.3 ° ) | 2.358 | 1.5e9 | 58.5 | 0.3 | 540 | 764 | 3.1e4 | 0.025 |
PKS 0227 − 369 new | 2.115 | 2e9 | 18.2 | 0.5 | 660 | 427 | 5.6e3 | 0.011 |
PKS 0227 − 369 old | 2.115 | 2e9 | 18.2 | 0.5 | 480 | 427 | 5.6e3 | 0.045 |
TXS 0458 − 020 new | 2.291 | 8e8 | 10.4 | 0.5 | 144 | 322 | 2.7e3 | 0.11 |
TXS 0458 − 020 quiesc. | 2.291 | 8e8 | 10.4 | 0.5 | 132 | 322 | 2.7e3 | 0.025 |
TXS 0458 − 020 “flare” | 2.291 | 8e8 | 10.4 | 0.5 | 192 | 322 | 2.7e3 | 0.35 |
TXS 0458 − 020 (Γ = 7) | 2.291 | 8e8 | 10.4 | 0.5 | 192 | 322 | 2.7e3 | 0.25 |
Notes. For the BLR we always assumed LBLR = 0.1Ld. For all models we assumed ψ = 0.1 = 5.7°, unless otherwise noted. For a simple geometry (a spherical torus surrounding the disk), the ratio LT/Ld corresponds to the aperture angle θT of the torus (the angle between the normal to the disk and the border of the torus): LT/Ld = cos2θT. A ratio LT/Ld = 0.3 gives θT = 57°, while LT/Ld = 0.5 gives θT = 45°.
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