How do recollimation-induced instabilities shape the propagation of hydrodynamic relativistic jets?

Open Access

Fig. 23.

Plot of $R = {\tilde{Φ}}_{m} (z = z^{*}, t = t_{l, 3 D}) / {\tilde{Φ}}_{m} (z = 1, t = t_{l, 3 D}) :$ $\mathcal{R} = \tilde{\Phi}_m(z=z^*,t=t_{l,\mathrm{3D}})/\tilde{\Phi}_m(z = 1,t=t_{l,\mathrm{3D}}):$ the mass flux of the fast jet, selected by Γ(z = z^*, t = t_l, 3D) > 2, normalized to the value at injection, for the various cases at the end of the simulations and at z^* = 15.

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