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Table 1.

Initial conditions of the simulated models.

Model pj ρj B ϕB vz ms Fj
code [pa] [ρa] [G] [deg] [c] [1043 erg s−1]
FMH1 1.0 0.01 0.42 70.7 0.87 1.12 4.8
FMH1_m4 1.0 0.01 0.42 70.7 0.87 1.12 4.8
FIH2 2.0 0.01 0.46 68.9 0.84 1.05 5.6
FIH3 3.0 0.01 0.49 67.3 0.81 1.01 6.1
FIH4 4.0 0.01 0.52 66.4 0.79 1.00 6.7
FMH1b 1.0 0.01 0.59 74.4 0.92 1.00 12.7
FMH1.3 1.3 0.05 0.55 67.8 0.82 1.00 6.3
FKS1 1.0 0.1 0.39 61.3 0.64 1.00 2.54
FML1 1.0 0.001 0.56 75.3 0.93 1.01 12.5
FMH1c 1.0 0.01 0.68 75.3 0.93 1.00 17.8
FIH3b 3.0 0.01 0.13 60.6 0.61 1.04 1.6
FMH0.3 0.3 0.05 0.66 72.7 0.90 1.03 12.4

NIH4 4.0 0.01 0.29 89.9 0.70 1.06 3.6
NIH1 1.0 0.01 0.22 88.2 0.75 1.09 1.6

Notes. Column 1: model names; Col. 2: initial jet thermal overpressure factor; Col. 3: initial jet density with respect to the ambient one; Col. 4: initial magnetic field strength in G; Col. 5: initial magnetic pitch angle; Col. 6: initial axial velocity; Col. 7: average initial Magnetosonic number; Col. 8: total jet flux in units of 1043 erg s−1. The model names obey the following logic. i) The first letter is for the magnetic field configuration: F for force-free and N for nonforce-free. ii) The second letter is for the dominant energy channel: M for magnetic, I for internal, and K for kinetic. iii) The third letter is for the jet density: S for ρj ≥ 0.1 ρa, H for 0.01 ρa ≤ ρj < 0.1 ρa, and L for ρj < 0.01 ρa. iv) The last number is the same as the jet thermal overpressure factor at injection. In the case of two models with the same nomenclature, we add a letter in progressively alphabetical order at the end of the name. Models with _m4 have the shear layer exponent set to m = 4 while for all the other models the exponent is m = 8.

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