Most relevant parameters for the two models investigated.
|External medium||Inner jet||Outer jet||Structured jet|
|CZase||p 0||η ρ,in||ℳc, in||η ρ, out||ℳc, out||L k, in / L k, total||L k, out / L k, total||Two-component jet|
|A||5 × 10-2||4.5 × 10-4||1.22||1||0.0||No|
|B||1 × 10-3||5 × 10-1||4.34||5 × 10-6||1.16||0.95||0.05||Yes|
|C||5 × 10-2||5 × 10-3||1.22||5 × 10-1||16.34||0.70||0.30||Yes|
|D||1 × 10-3||5 × 10-6||1.22||1 × 10-1||6||0.25||0.75||Yes|
|E||5 × 10-2||5 × 10-3||1.22||5 × 10||19.0||5 × 10-3||0.995||Yes|
|F||5 × 10-2||1 × 10-3||0||5 × 10-2||6.0||0||1||Yes|
Notes. In addition to these values, the external medium has a normalized number density ρ0 = 1 and a normalized pressure p0 ≃ 5 × 10-2 or p0 ≃ 1 × 10-3 (these two types of pressure are chosen according to the energy ratio between inner and outer jet components). The inner jet always presents an initial Lorentz factor of γ = 10, higher than that of the outer jet initialized at γ = 3. The outer jet is assumed to be in pressure equilibrium with the external medium ηp, out = 1, contrary to the inner jet which presents a larger pressure ηp, in = 1.5.
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