---------------

[lcc]{} & $\phi_{\bar{\nu}_e}$(fin) & Pattern\
\
NH-A & $|U_{e1}|^2 \phi_{\bar{\nu}_e} + (1-|U_{e1}|^2) \phi_{\bar{\nu}_x}$ & (B)\
IH-A & $|U_{e3}|^2 \phi_{\bar{\nu}_e} + (1-|U_{e3}|^2) \phi_{\bar{\nu}_x}$ & (C)\
NA-NA and IA-NA & $|U_{e1}|^2 \phi_{\bar{\nu}_e} + (1-|U_{e1}|^2) \phi_{\bar{\nu}_x}$ & (B)\
\
NH-A & $|U_{e1}|^2 \phi_{\nu_x} + |U_{e2}|^2 \phi_{\bar{\nu}_x}
+ |U_{e3}|^2 \phi_{\bar{\nu}_x}$ & (C)\
NH-NA & $|U_{e1}|^2 \phi_{\nu_x} + |U_{e2}|^2 \phi_{\bar{\nu}_x}
+ |U_{e3}|^2 \phi_{\bar{\nu}_x}$ & (C)\
IH-A & $|U_{e1}|^2 \phi_{\nu_e} + |U_{e2}|^2 \phi_{\bar{\nu}_x}
+ |U_{e3}|^2 \phi_{\bar{\nu}_e}$ & (A)\
IH-NA & $|U_{e1}|^2 \phi_{\bar{\nu}_e} + |U_{e2}|^2 \phi_{\bar{\nu}_x}
+ |U_{e3}|^2 \phi_{\nu_e}$ & (B)\
\
NH-A & $|U_{e1}|^2 \phi_{\bar{\nu}_e} + |U_{e2}|^2 \phi_{\bar{\nu}_x}
+ |U_{e3}|^2 \phi_{\nu_e}$ & (B)\
NH-NA & $|U_{e1}|^2 \phi_{\bar{\nu}_e} + |U_{e2}|^2 \phi_{\bar{\nu}_x}
+ |U_{e3}|^2 \phi_{\nu_e}$ & (B)\
IH-A & $|U_{e1}|^2 \phi_{\bar{\nu}_x} + |U_{e2}|^2 \phi_{\bar{\nu}_x}
+ |U_{e3}|^2 \phi_{\nu_x}$ & (C)\
IH-NA & $|U_{e1}|^2 \phi_{\nu_x} + |U_{e2}|^2 \phi_{\bar{\nu}_x}
+ |U_{e3}|^2 \phi_{\bar{\nu}_x}$ & (C)\

SN neutrinos change their flavors by the RSF conversion and the MSW effect in SN ejecta. The flavor changes depend on the distributions of the density and electron fraction. Here we investigate the dependence of neutrino energy spectra and the neutrino signals on the neutrino oscillation parameters and the electron fraction.

![image](f9a.eps){width="6.7cm"} ![image](f9b.eps){width="6.7cm"}

In this section, we consider the dependence on the mass hierarchies, electron fraction 