\begin{table}%t2 \caption{\label{table2}Parameter values adopted to compute the SEDs for the three emitting zones$^{(\dag)}$.} %\centerline { \small \begin{tabular}{lcccccccc} \hline \hline\noalign{\smallskip} \it{Parameter} & \multicolumn{2}{c}{Fig.~\ref{fig2}} & \multicolumn{2}{c}{Fig.~\ref{fig3}} & \multicolumn{2}{c}{Fig.~4} & \multicolumn{ 2}{c}{Fig.~\ref{fig5}} \\ \hline\\[-1.8mm] Jet kinetic power $Q_{\rm jet}$ (erg~s~$^{-1}$ ) & \multicolumn{4}{c}{$10^{36}$} & \multicolumn{4}{c}{$10^{37}$} \\ %\hline ISM density $n_{\rm ISM}$ (cm$^{-3}$) & \multicolumn{2}{c}{0.1} & \multicolumn{2}{c}{$1$} & \multicolumn{2}{c}{0.1} & \multicolumn{2}{c}{1}\\ Source age $t_{\rm MQ}$ (yr) & $10^{4}$ & $10^{5}$ & $10^{4}$ & $10^{5}$ & $10^{4}$ & $10^{5}$ & $10^{4}$ & $10^{5}$ \\ \hline {\it SHELL} & \multicolumn{7} {}{} & {} \\ %\hline Magnetic field $B$ (G) & 2.9 $\times 10^{-5}$ & 1.1 $\times 10^{-5}$ & 5.8 $\times 10^{-5}$ & 2.3 $\times 10^{-5}$ & 4.6 $\times 10^{-5}$ & 1.8 $\times 10^{-5}$ & 9.2 $\times 10^{-5}$ & $3.6 \times 10^{-5}$ \\ Shock velocity $v_{\rm b}$ (cm s$^{-1}$) & $4.3\times 10^{7}$ & $1.7 \times 10^{7}$ & $2.7 \times 10^{7}$ & $1.0 \times 10^{7}$ & $6.9 \times 10^{7}$ & $2.7 \times 10^{7}$ & $4.3 \times 10^{7}$ & $1.7 \times 10^{7}$ \\ Emitter size $r$ (cm) & $2.3 \times 10^{19}$ & $9.1 \times 10^{19}$ & 1.4 $\times 10^{19}$ & $5.7 \times 10^{19}$ & $3.62 \times 10^{19}$ & $1.44 \times 10^{20}$ & 2.3 $\times 10^{19}$ & $9.1 \times 10^{19}$ \\ Rad. energy dens. $u_{\star}$ (erg cm$^{-3}$) & $5.0 \times 10^{-12}$ & $3.2 \times 10^{-11}$ & 1.2 $\times 10^{-13}$ & $8.0 \times 10^{-13}$ & 2.0 $\times 10^{-12}$ & $1.3 \times 10^{-12}$ & 5.0 $\times 10^{-13}$ & $3.2 \times 10^{-13}$ \\ Maximum energy $E_{\rm max}$ (TeV) & 8.1 & 5.1 & 3.6 & 2.3 & 10.2 & 6.4 & 4.5 & 2.8 \\ Target density $n_{\rm t}$ (cm$^{-3}$) & 0.4 & 0.4 & 4.0 & 4.0 & 0.4 & 0.4 & 4.0 & 4.0\\ \hline {\it COCOON} & \multicolumn{7} {}{} & {} \\ %\hline Magnetic field $B$ (G) & 3.8 $\times 10^{-5}$ & 1.5 $\times 10^{-5}$ & $7.5 \times 10^{-5}$ & $3.0 \times 10^{-5}$ & 5.9 $\times 10^{-5}$ & $2.4 \times 10^{-5}$ & $1.2 \times 10^{-4}$ & $4.7 \times 10^{-5}$ \\ Shock velocity $v_{\rm s}$ (cm s$^{-1}$) & $1.8 \times 10^{10}$ & $1.8 \times 10^{10}$ & $1.8 \times 10^{10}$ & 1.8 $\times 10^{10}$ & $1.8 \times 10^{10}$ & $1.8 \times 10^{10}$ & $1.8 \times 10^{10}$ & $1.8 \times 10^{10}$ \\ Emitter size $r$ (cm) & $6.5 \times 10^{18}$ & $2.5 \times 10^{18}$ & $4.0 \times 10^{19}$ & 1.6 $\times 10^{19}$ & $1.0 \times 10^{19}$ & $4.0 \times 10^{18}$ & $6.5 \times 10^{19}$ & 2.5 $\times 10^{19}$ \\ Rad. energy dens. $u_{\star}$ (erg cm$^{-3}$) & $7.0 \times 10^{-12}$ & $1.7 \times 10^{-11}$ & 4.4 $\times 10^{-13}$ & $1.1 \times 10^{-12}$ & $2.8 \times 10^{-12}$ & $1.7 \times 10^{-12}$ & 7.0 $\times 10^{-13}$ & $4.4 \times 10^{-13}$ \\ Maximum energy $E_{\rm max}$ (TeV) & 275.5 & 275.5 & 275.5 & 275.5 & 871.2 & 871.2 & 871.23 & 871.2 \\\hline {\it RECONFINEMENT} & \multicolumn{7} {}{} & {} \\ %\hline Magnetic field $B$ (G) & $2.6 \times 10^{-5}$ & $1.0 \times 10^{-5}$ & $5.2 \times 10^{-5}$ & $2.1 \times 10^{-5}$ & $4.2 \times 10^{-5}$ & $1.6 \times 10^{-5}$ & $8.3 \times 10^{-5}$ & $3.3 \times 10^{-5}$ \\ Shock velocity $v_{\rm conf}$ (cm s$^{-1}$) & 1.8 $\times 10^{9}$ & $1.8 \times 10^{9}$ & 1.8 $\times 10^{9}$ & $1.8 \times 10^{9}$ & $1.8 \times 10^{9}$ & $1.8 \times 10^{9}$ & $1.8 \times 10^{9}$ & $1.8 \times 10^{9}$ \\ Emitter size $r$ (cm) & $1.9 \times 10^{19}$ & $7.6 \times 10^{19}$ & $1.2 \times 10^{19}$ & $4.8 \times 10^{19}$ & $3.0 \times 10^{19}$ & $1.2 \times 10^{20}$ & $1.9 \times 10^{19}$ & $7.6 \times 10^{19}$ \\ Rad. energy dens. $u_{\star}$ (erg cm$^{-3}$) & $2.5 \times 10^{-8}$ & $4.0 \times 10^{-9}$ & $1.0 \times 10^{-7}$ & $1.6 \times 10^{-8}$ & $6.4 \times 10^{-9}$ & $1.0 \times 10^{-9}$ & $2.5 \times 10^{-8}$ & $4.0 \times 10^{-9}$ \\ Maximum energy $E_{\rm max}$ (TeV) & 3.2 & 3.2 & 3.2 & 3.2 & 10.1 & 10.1 & 10.1 & 10.1 \\ \hline \end{tabular}} \smallskip%\medskip $^{(\dag)}$ The target density, $n_{\rm t}$, is only shown when non-negligible. We show the parameter values at $t_{\rm MQ}$, but we note that they vary smoothly with time. The computation of the non-thermal particle distribution has taken this into account. See Sect.~2 for details. \end{table}