All Figures

$\begin{figure} \par\includegraphics[width=7.7cm,clip]{7123fig1.eps} \end{figure}$ Figure 1: Nuclear mass fraction profiles of ⁴He, ¹²C, ¹⁶O, ²⁸Si, ³²S, ⁵²Fe and ⁵⁶Ni for a detonation front in pure ¹²C at T=10⁸ K and $\rho = 10^8$ g cm^-3. Z is the distance to the shock in cm. The thin solid lines give the steady state solution of the ZND model. The heavy dots (the density of the dots is so high that they form thick curves) are obtained with the time-dependent calculations with two different resolutions (mesh size 10^-4 cm and 10 cm).
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In the text

$\begin{figure} \par\includegraphics[width=7.8cm,clip]{7123fig2.eps} \end{figure}$ Figure 2: Same as Fig. 1, but with screening effects taken into account. Results only obtained with the time-dependent calculations for four resolutions (from left to right: mesh size 10^-3 cm, 0.1 cm, 1 cm and 10 cm).
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In the text

$\begin{figure} \par\includegraphics[width=8cm,clip]{7123fig3.eps} \end{figure}$ Figure 3: Temperature (in K), velocity (in cm s^-1), density (in g cm^-3) and pressure (in erg cm^-3) profiles of a detonation front in pure ¹²C at T=10⁸ K and $\rho = 10^8$ g cm^-3 at time = $5 \times 10^{-6}$ s. X is in cm.
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In the text

$\begin{figure} \par\includegraphics[width=8cm,clip]{7123fig4.eps} \end{figure}$ Figure 4: Same as Fig. 3, but at time = $6 \times 10^{-10}$ s with a resolution of 10^-3 cm.
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In the text

$\begin{figure} \par\includegraphics[width=7.9cm,clip]{7123fig5.eps} \end{figure}$ Figure 5: Nuclear energy generation (erg g^-1 s^-1) profile of a detonation front in pure ¹²C at T=10⁸ K and $\rho = 10^8$ g cm^-3 at time = $6 \times 10^{-10}$ s with a resolution of 10^-3 cm. X is in cm.
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In the text

$\begin{figure} \par\includegraphics[width=8cm,clip]{7123fig6.eps} \end{figure}$ Figure 6: Same as Fig. 3, but at time = $7 \times 10^{-6}$ s and for a mixture $X_{ ^{12}{\rm C}} = 0.3$ and $X_{ ^{52}{\rm Fe}} = 0.7$ .
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In the text

$\begin{figure} \par\includegraphics[width=7.7cm,clip]{7123fig7.eps} \end{figure}$ Figure 7: Nuclear mass fraction profiles of a detonation front in a mixture $X_{ ^{12}{\rm C}} = 0.3$ and $X_{ ^{52}{\rm Fe}} = 0.7$ at T=10⁸ K and $\rho = 10^8$ g cm^-3 at time = $7 \times 10^{-6}$ s. Z is the distance to the shock in cm.
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In the text

$\begin{figure} \par\includegraphics[width=7.8cm,clip]{7123fig2.eps} \end{figure}$	Figure 2: Same as Fig. 1, but with screening effects taken into account. Results only obtained with the time-dependent calculations for four resolutions (from left to right: mesh size 10^-3 cm, 0.1 cm, 1 cm and 10 cm).
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$\begin{figure} \par\includegraphics[width=8cm,clip]{7123fig3.eps} \end{figure}$	Figure 3: Temperature (in K), velocity (in cm s^-1), density (in g cm^-3) and pressure (in erg cm^-3) profiles of a detonation front in pure ¹²C at T=10⁸ K and $\rho = 10^8$ g cm^-3 at time = $5 \times 10^{-6}$ s. X is in cm.
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$\begin{figure} \par\includegraphics[width=8cm,clip]{7123fig4.eps} \end{figure}$	Figure 4: Same as Fig. 3, but at time = $6 \times 10^{-10}$ s with a resolution of 10^-3 cm.
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$\begin{figure} \par\includegraphics[width=7.9cm,clip]{7123fig5.eps} \end{figure}$	Figure 5: Nuclear energy generation (erg g^-1 s^-1) profile of a detonation front in pure ¹²C at T=10⁸ K and $\rho = 10^8$ g cm^-3 at time = $6 \times 10^{-10}$ s with a resolution of 10^-3 cm. X is in cm.
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$\begin{figure} \par\includegraphics[width=8cm,clip]{7123fig6.eps} \end{figure}$	Figure 6: Same as Fig. 3, but at time = $7 \times 10^{-6}$ s and for a mixture $X_{ ^{12}{\rm C}} = 0.3$ and $X_{ ^{52}{\rm Fe}} = 0.7$ .
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$\begin{figure} \par\includegraphics[width=7.7cm,clip]{7123fig7.eps} \end{figure}$	Figure 7: Nuclear mass fraction profiles of a detonation front in a mixture $X_{ ^{12}{\rm C}} = 0.3$ and $X_{ ^{52}{\rm Fe}} = 0.7$ at T=10⁸ K and $\rho = 10^8$ g cm^-3 at time = $7 \times 10^{-6}$ s. Z is the distance to the shock in cm.
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