similar $T_{\rm max} - \rho_{\rm max}$ distribution; the compression and the maximum temperature are roughly linear functions of the unburned density.

Figure 6 shows a significant dispersion in the $T_{\rm max} - \rho_{\rm max}$ distribution around the mean value, reaching nearly one order of magnitude in $\rho_{\rm max}$ for given $T_{\rm max}$, at $T_{{\rm max}, 9} \lsim 5$. This is a unique behavior in the multi-D models, potentially leading to a variety of burning products otherwise not expected in strictly spherically symmetric models like W7.

The different hydrodynamic properties lead to different amounts of material as a function of $T_{\rm max}$ (or $\rho_{\rm max}$), and this is the main reason why different nucleosynthesis features appear. Figure 8 shows the mass of the material as a function of $T_{\rm max}$. It is seen that the deflagration is efficient in W7, and thus the W7 model has a much larger amount of the mass with $T_{{\rm max}, 9} \gsim 6$ than the 2D models. At $T_{{\rm max}, 9} \lsim 3 - 4$, there appears a peak in the C-DDT model; this is due to the detonation wave burning the fuel material left behind the deflagration stage. The O-DDT model shows a characteristic 