at nonadiabatic RSF-X resonance. Thus, we see no effects in the conversions between $\bar{\nu}_2$ and $\nu_3$. The $\nu_3$ corresponds to $\nu_{\mu,\tau}$ and a small fraction of $\nu_e$. The $\nu_2$ is the mixed flavor eigenstates of 70 % of $\bar{\nu}_{\mu,\tau}$ and 30 % of $\bar{\nu}_e$ in vacuum.

Third, we consider the case of the inverted mass hierarchy and $Y_e = 0.49$ in the inner region. Figure 6 shows the conversion probabilities from $\nu_e$ \[6(a)\] and $\bar{\nu}_{\mu,\tau}$ \[6(b)\]. RSF-H conversion occurs between $\nu_e$ and $\bar{\nu}_{\mu,\tau}$ similarly to the second case. Flavor conversion occurs at RSF-H and MSW-H resonances for the original $\nu_e$. It occurs at RSF-H and MSW-L resonances for the original $\bar{\nu}_{\mu,\tau}$.

The flavor eigenstate $\nu_e$ corresponds to $\nu_1$ at high density limit. The mass eigenstate $\nu_1$ does not convert at RSF-H resonance. It converts to $\bar{\nu}_1$ at RSF-L resonance because of nonadiabaticity of this resonance. Therefore, the neutrinos originally produced as $\nu_e$ appear as $\bar{\nu}_1$, corresponding to the mixtures of 70 % of $\bar{\nu}_e$ and 30 % of $\bar{\nu}_{\mu,\tau}$ in vacuum. The flavor eigenstate $\bar{\nu}_{\mu,\tau}$ is a mixed state of $\nu_2$ and $\bar{\nu}_2$. There are no resonances for $\bar{\nu}_2$. The $\nu_2$ has RSF-H and MSW-L resonances. Since both of the 