All Figures

$\begin{figure} \par\resizebox{8.8cm}{!}{\includegraphics[width=8.8cm]{5395fig1.eps}} \end{figure}$ Figure 1: Influence of the value of $t_{\rm obs}$ parameter on the time averaged SED (left panel) with $\Delta t_{\rm obs}=4 t_{\rm inj}$ and $t_{\rm crit}=0.5 t_{\rm inj}$ . Vertical dashed lines represent location of the frequency break $\nu _{\rm break}$ calculated for each previous curve (see Eq. (6)). Resulting local spectral indices in normalized frequency range [-0.5,0] (upper solid curve), [-1,-0.5] (lower solid curve) and [-1,0] (dashed curve) are given on the right panel.
Open with DEXTER

In the text

$\begin{figure} \par\resizebox{8.8cm}{!}{\includegraphics{5395fig2.eps}} \end{figure}$ Figure 2: Same as Fig. 1 for the influence of the $\Delta t_{\rm obs}$ parameter with $t_{\rm obs}=t_{\rm crit}=0.5 t_{\rm inj}$ . Considering these parameter values, we easily verify that spectral index above $\nu_{\rm break}=0.25~\nu_{\rm smax,0}$ is going to be flat since $\Delta t_{\rm obs}\geqslant t_{\rm inj}-t_{\rm obs}=0.5$ .
Open with DEXTER

In the text

$\begin{figure} \par\resizebox{8.8cm}{!}{\includegraphics{5395fig3.eps}} % \end{figure}$ Figure 3: Fits of Markarian 501 UV/X-ray synchrotron spectrum for three different periods.
Open with DEXTER

In the text

$\begin{figure} \par\resizebox{8.8cm}{!}{\includegraphics{5395fig2.eps}} \end{figure}$	Figure 2: Same as Fig. 1 for the influence of the $\Delta t_{\rm obs}$ parameter with $t_{\rm obs}=t_{\rm crit}=0.5 t_{\rm inj}$ . Considering these parameter values, we easily verify that spectral index above $\nu_{\rm break}=0.25~\nu_{\rm smax,0}$ is going to be flat since $\Delta t_{\rm obs}\geqslant t_{\rm inj}-t_{\rm obs}=0.5$ .
Open with DEXTER

$\begin{figure} \par\resizebox{8.8cm}{!}{\includegraphics{5395fig3.eps}} % \end{figure}$	Figure 3: Fits of Markarian 501 UV/X-ray synchrotron spectrum for three different periods.
Open with DEXTER