Table 1: The main parameters adopted in our calculations.
    ${{\rm Jet}\: A}$ ${{\rm Jet}\: B}$
$\rm {Symbols}$ ${\rm Definitions\: of\: the\: Symbols}$ ${\rm Forward\: Shock}$ ${\rm Forward\: Shock}$ ${\rm Reverse\: Shock}$
$E^l_{\rm iso}\:(\rm {erg})$ $\rm {Isotropic\: Energy}$ $5.8\times 10^{52}$ $1.0\times10^{54}$
$\Gamma_l$ $\rm {Initial\:Lorentz\:Factor}$ 300 300
$n_1\:(\rm {cm^{-3}})$ $\rm {Number\: Density\:of\: ISM}$ 50.0 50.0
pl $\rm {Electron\: Spectral\: Index}$ 2.10 2.12
$\theta_l$ $\rm {Half\:Opening\:Angle}$ 0.08 0.04
$\Delta\theta_l$ $\rm {Viewing\:Angle}$ 0.07 0.05
$\varepsilon^l_i$ $\rm {Radiative\: Efficiency}$ 0.0 0.0 0.0
$\epsilon^l_{{\rm e},i}$ $\rm {Electron\:Equipartition\:Factor}$ 0.05 0.1 0.1
$\epsilon^l_{B,i}$ $\rm {Magnetic\:Equipartition\:Factor}$ 0.0008 0.01 0.01
  ${{\rm Values\:Of\:Following\: Physical\:Quantities\:At}\:t\sim3000\:\rm s}$
$\gamma^l_i$ $\rm {Bulk\:Lorentz\:Factor}$ 22 29 32
$\gamma^l_{{\rm m},i}$ $\rm {Minimal\:Lorentz\:Factor}$ 180 540 3.5
$\gamma^l_{{\rm c},i}$ $\rm {Cooling\:Lorentz\:Factor}$ 2600 205 3.5
$\gamma^l_{{\rm M},i}$ $\rm {Maximal\:Lorentz\:Factor}$ $7.6\times 10^{7}$ $3.6\times 10^{7}$ $4.8\times 10^{7}$
$B^l_i\: (\rm {G})$ $\rm {Comoving\:Magnetic\:Field\:Strength}$ 1.7 7.8 4.3
$m^l_i\: (\rm {g})$ $\rm {Shocked\:Mass}$ $1.2\times 10^{29}$ $5.2\times 10^{29}$ $3.7\times 10^{30}$
Notes: for Jet A, l=A and for Jet B, l=B. The subscript i=2 represents forward-shocked region and i=3 represents reverse-shocked region. In the lower part of the table, some physical quantities involved in the calculations at ${t\sim 3000}$ s are presented for illustration.


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