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$\begin{figure} \par\includegraphics[width=6.7cm,clip]{Graph1.eps} \end{figure}$ Figure 1: The plots of log $(\nu f_{\nu})_{\rm p}- \log~\nu_{\rm p}$ for the bremsstrahlung (open circle), Comptonized (open triangle), synchrotron (open square), and the GRB model (filled triangle) radiation, where log $(\nu f_{\nu ,i})_{\rm p}$ represents log $(\nu f_{\nu ,\rm B})_{\rm p}$ , log $(\nu f_{\nu ,\rm C})_{\rm p}$ , log $(\nu f_{\nu ,\rm S})_{\rm p}$ and log $(\nu f_{\nu ,\rm G})_{\rm p}$ , while log $(\nu _{\rm p}/\nu _{0,i})$ represents log $(\nu _{\rm p}/\nu _{0,\rm B})$ , log $(\nu _{\rm p}/\nu _{0,\rm C})$ , log $(\nu _{\rm p}/\nu _{0,\rm S})$ and log $(\nu _{\rm p}/\nu _{0,\rm P})$ . The data are taken from Tables 1-4.
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In the text

$\begin{figure} \par\includegraphics[width=6.7cm,clip]{Graph2.eps} \end{figure}$ Figure 2: The plot of log $(\nu f_{\nu,\rm B})- \log~\Gamma$ for the bremsstrahlung radiation at various frequencies (the solid lines from the bottom to the top: log $(\nu/\nu_{0,\rm B})=-4,\;-2,0$ ; the dashed line: log $(\nu /\nu _{0,\rm B})=2$ ; the dotted line: log $(\nu /\nu _{0,\rm B})=3$ ; the dashed and dotted line: log $(\nu /\nu _{0,\rm B})=4$ ; the dashed dotted dotted line: log $(\nu /\nu _{0,\rm B})=5$ ).
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In the text

$\begin{figure} \par\includegraphics[width=6.7cm,clip]{Graph3.eps} \end{figure}$ Figure 3: The plot of log $(\nu f_{\nu,\rm C})- \log~\Gamma$ for the Comptonized radiation at various frequencies (the solid lines from the bottom to the top: log $(\nu/\nu_{0,\rm C})=-4,\;-2,0$ ; the dashed line: log $(\nu /\nu _{0,\rm C})=2$ ; the dotted line: log $(\nu /\nu _{0,\rm C})=3$ ; the dashed and dotted line: log $(\nu /\nu _{0,\rm C})=4$ ; the dashed dotted dotted line: log $(\nu /\nu _{0,\rm C})=5$ ).
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In the text

$\begin{figure} \par\includegraphics[width=6.7cm,clip]{Graph4.eps} \end{figure}$ Figure 4: The plot of log $(\nu f_{\nu,\rm S})- \log~\Gamma$ for the synchrotron radiation at various frequencies (the solid lines from the bottom to the top: log $(\nu/\nu_{0,\rm S})=0,\;2,\;4$ ; the dashed line: log $(\nu /\nu _{0,\rm S})=6$ ; the dotted line: log $(\nu /\nu _{0,\rm S})=8$ ; the dashed and dotted line: log $(\nu /\nu _{0,\rm S})=9$ ; the dashed dotted dotted line: log $(\nu /\nu _{0,\rm S})=10$ ).
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In the text

$\begin{figure} \par\includegraphics[width=6.7cm,clip]{Graph5.eps} \end{figure}$ Figure 5: The plot of log $(\nu f_{\nu,\rm G})- \log~\Gamma$ for the radiation bearing the GRB form at various frequencies (the solid lines from the bottom to the top: log $(\nu/\nu_{0,\rm G})=-4,\;-2,\;0,\;2$ ; the dotted line: log $(\nu /\nu _{0,\rm G})=4$ ; the dashed line: log $(\nu /\nu _{0,\rm G})=6$ ; the dashed and dotted line: log $(\nu /\nu _{0,\rm G})=8$ ).
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In the text

$\begin{figure} \par\includegraphics[width=6.7cm,clip]{Graph5.eps} \end{figure}$	Figure 5: The plot of log $(\nu f_{\nu,\rm G})- \log~\Gamma$ for the radiation bearing the GRB form at various frequencies (the solid lines from the bottom to the top: log $(\nu/\nu_{0,\rm G})=-4,\;-2,\;0,\;2$ ; the dotted line: log $(\nu /\nu _{0,\rm G})=4$ ; the dashed line: log $(\nu /\nu _{0,\rm G})=6$ ; the dashed and dotted line: log $(\nu /\nu _{0,\rm G})=8$ ).
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