$\begin{figure} \par\includegraphics[width=8.5cm,clip]{2853_f1.eps}\end{figure}$ Figure 1: Radial profile of the normal ( $B_{\rm r}$ ) and tangential ( $B_{\rm t}$ ) components of the magnetic field in a test-particle self-similar model. Each component is normalized to the forward shock.
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In the text

$\begin{figure} \par\includegraphics[width=8.5cm,clip]{2853_f2.eps} \end{figure}$ Figure 2: Magnetic field radial profile for different values of the injection efficiency, $\eta _{{\rm inj}}$ , when the hydrodynamics is coupled with the non-linear DSA model. The width of the shocked region is smaller and smaller as the feedback of the accelerated particles on the SNR dynamicsincreases.
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In the text

$\begin{figure} \par\includegraphics[width=8.5cm,clip]{2853_f3.eps}\par\includegraphics[width=8.5cm,clip]{2853_f4.eps}\end{figure}$ Figure 3: Radio (top panel) and X-ray (bottom panel) synchrotron volume emissivity, $\epsilon _{\nu }$ , radial profile for different injection efficiencies.
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In the text

$\begin{figure} \par\includegraphics[width=8.5cm,clip]{2853_f5.eps}\par\includegraphics[width=8.5cm,clip]{2853_f6.eps}\end{figure}$ Figure 4: Radio (top panel) and X-ray (bottom panel) synchrotron volume emissivity radial profile after projection onto the line-of-sight for different injection efficiencies. Emission from particles accelerated at the reverse shock is assumed to be negligible.
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In the text

$\begin{figure} \par\includegraphics[width=8.5cm,clip]{2853_f1.eps}\end{figure}$	Figure 1: Radial profile of the normal ( $B_{\rm r}$ ) and tangential ( $B_{\rm t}$ ) components of the magnetic field in a test-particle self-similar model. Each component is normalized to the forward shock.
Open with DEXTER

$\begin{figure} \par\includegraphics[width=8.5cm,clip]{2853_f2.eps} \end{figure}$	Figure 2: Magnetic field radial profile for different values of the injection efficiency, $\eta _{{\rm inj}}$ , when the hydrodynamics is coupled with the non-linear DSA model. The width of the shocked region is smaller and smaller as the feedback of the accelerated particles on the SNR dynamicsincreases.
Open with DEXTER

$\begin{figure} \par\includegraphics[width=8.5cm,clip]{2853_f3.eps}\par\includegraphics[width=8.5cm,clip]{2853_f4.eps}\end{figure}$	Figure 3: Radio (top panel) and X-ray (bottom panel) synchrotron volume emissivity, $\epsilon _{\nu }$ , radial profile for different injection efficiencies.
Open with DEXTER

$\begin{figure} \par\includegraphics[width=8.5cm,clip]{2853_f5.eps}\par\includegraphics[width=8.5cm,clip]{2853_f6.eps}\end{figure}$	Figure 4: Radio (top panel) and X-ray (bottom panel) synchrotron volume emissivity radial profile after projection onto the line-of-sight for different injection efficiencies. Emission from particles accelerated at the reverse shock is assumed to be negligible.
Open with DEXTER