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Table 1

Parameters of the pulsed cylindrical jet simulations (Sect. 3).

Fixed parameters (from Lee et al. 2001)
One-sided jet mass-loss rate
Jet semi-opening angle θj = 0o
Jet radius Rj = 2.5 × 1015 cm
Mean jet velocity v0 = 120 km s–1
Jet velocity variation
Semi-amplitude ΔV = 60 kms–1
Jet density variation ρj(t) = ρj0 [v0/vj(t)] (constant mass-flux)
Jet density at t = 0 ρj0 = 1.6 × 10-20gcm3
Jet temperature Tj = 270 K
Ambient core temperature Ta = 30K
Radiative cooling function Λ(270 K ≤ T < 104 K) from Dalgarno & McCray (1972)
Λ(T ≥ 104 K) from MacDonald & Bailey (1981)
Simulation domain (R, z) = (7.0 × 1016 cm, 1.4 × 1017 cm) = (4679 au, 9358 au)
Number of cells nR × nz = 336 × 672
Resolution ΔR = Δz = 2.08 × 1014 cm = 14 au
Variable parameters
Model name PCJ-U(a) PCJ-Z PCJ-R PCJ-RW(b)
(Fig. 1a) (Fig. 1b) (Fig. 1c) (Fig. 2)
Core density profile Uniform z-stratified Flattened singular core
ρa(r) ρa0
Core density at z = 0, R = 2.5 × 1015 cm ρa0 = 1.6 × 10–20gcm–3 1.6 × 10–18gcm–3
Core/jet density contrast at z = 0 n = ρj0/ρa0 = 1 0.01
Jet variability period P = 310 yr 115 yr
Simulation age t = 610 yr 296 yr

Notes. (a)Identical parameters to pulsed jet simulation of Lee et al. (2001) (see their Fig. 7). (b)Identical parameters to pulsed wind simulation of Lee et al. (2001) (cf. their Fig. 12), except that the wide-angle wind is replaced here by a cylindrical jet of same mass-flux, injection radius, and velocity variability.

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