Table B.2.
Fit parameters for the broken power law fits to the jet width for the western and eastern jets shown in Fig. 5.
| Fit to | W0 | σW0 | ku | σku | kd | σku | zB | σzB | χ2 |
|---|---|---|---|---|---|---|---|---|---|
| W jet - all | 0.27 | 0.02 | 0.42 | 0.02 | 1.20 | 0.05 | 2.7 | 0.2 | 2.59 |
| W jet - Baczko et al. 22 | 0.26 | 0.02 | 0.21 | 0.05 | 1.22 | 0.05 | 2.66 | 0.22 | 1.91 |
| W jet - high freq | 0.26 | 0.03 | 0.42 | 0.02 | 1.26 | 0.19 | 2.7 | 0.4 | 3.99 |
| E jet - all | 0.22 | 0.03 | 0.50 | 0.02 | 0.75 | 0.01 | 1.10 | 0.23 | 2.35 |
| E jet - Baczko et al. 22 | 0.24 | 0.02 | 0.22 | 0.06 | 0.80 | 0.01 | 1.40 | 0.18 | 1.40 |
| E jet - high freq | 0.18 | 0.03 | 0.46 | 0.04 | 0.90 | 0.06 | 0.85 | 0.21 | 3.56 |
Notes. Column 1: Which data the fits describe: W stands for western jet and E for eastern. Column 2: Initial jet width. Column 3: Error on the initial jet width. Column 4: Upstream index. Column 5: Error on the upstream index. Column 6: Downstream index. Column 7: Error on the downstream index. Column 8: Transition distance. Column 9: Error on the transition distance. Column 10: Chi square for the fit.
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