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Table 1.
Main jet parameters for the runs as a function of the assumed αB boost factor in the Bondi accretion model (Eq. (1)).
| Parameter | Run B | Run C | Run D | Run E | Run F | Run 0 |
|---|---|---|---|---|---|---|
| αB | 1 | 3 | 10 | 30 | 50 | 0 |
| Pj [erg s−1] | 3 × 1043 | 9 × 1043 | 3 × 1044 | 9 × 1044 | 1.5 × 1045 | 0 |
| ṀBH/ṀEdd | 0.002 | 0.006 | 0.02 | 0.06 | 0.1 | 0 |
| Bav, j [μG] | 28.6 | 70.1 | 66.4 | 70.4 | 41.5 | 0 |
| Bmax, j [μG] | 49.8 | 106.9 | 91.2 | 109.0 | 97.6 | 0 |
| Tav, j [K] | 1.5 × 107 | 3.6 × 107 | 1.8 × 108 | 4.3 × 108 | 5.8 × 108 | 0 |
| vav, j [km s−1] | 260 | 1754 | 2750 | 3888 | 4215 | 0 |
| vmax, j [km s−1] | 424 | 2567 | 4355 | 10 286 | 7943 | 0 |
| NCRe | 2.7 × 1064 | 3.9 × 1064 | 6.7 × 1064 | 9.9 × 1064 | 1.2 × 1065 | 0 |
Notes. All quantities are measured 32 Myr after the injection of jets, and the average, total, or maximum quantities are taken from the distribution of tracer particles injected in jets.
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