The energies of positron and electron are evaluated as E$_{e}$ + = E$_{ν}$ + m$_{p}$ − m$_{n}$ − m$_{e}$$_{+}$ for ¯ ν$_{e}$ + p → n + e + and E$_{e}$ = E$_{ν}$ − m$_{e}$ 2 for ν + e − → ν + e $^{−}$, respectively. The cross sections of the above four reactions are adopted from [59]. The mass of SNO is 1000 ton and the solvent is heavy water. SNO detects not only ¯ ν$_{e}$ events but also ν$_{e}$ events with charged and neutral current reactions. As for the efficiency of the detector, we assumed as follows for simplicity: η$_{(}$$_{E}$$_{e}$$_{)}$ = 0 for E$_{e}$ < 5 MeV and η$_{(}$$_{E}$$_{e}$$_{)}$ = 1 for E$_{e}$ ≥ 5 MeV [62]. We evaluate the ¯ ν$_{e}$ and ν$_{e}$ event numbers using the four reactions, ν$_{e}$ + d → p + p + e − (13) ¯ ν$_{e}$ + d → n + n + e + (14) ν + d → p + n + ν (15) ν + e → ν + e $^{−}$. (16) The main reactions of ¯ ν$_{e}$ and ν$_{e}$ are the first and second reactions, respectively [63]. The cross sections of these reactions are adopted from [64]. The cross sections become larger as the neutrino energy increases. Although the SNO experiment has already ended, we also evaluate the neutrino events by SNO because the detection efficiency of ν$_{e}$ is high and similar in next generation detector like SNO. We calculate the survival probabilities of ν$_{e}$ and ¯ ν$_{e}$ from the supernova, P ( E$_{ν}$ ) and ¯ P ( E$_{ν}$ ). Figure 2 shows the calculated results. Left panels of Figure 2 are P ( E$_{ν}$ ) in the case of normal hierarchy in every 1 s, and right panels of Figure 2 are ¯ P ( E$_{ν}$ ) in the case of inverted hierarchy. Red, green, blue, purple, sky blue and orange lines correspond to the results in t = 0, 1, 2, 3, 4 and 5 s after core bounce. We showed the results for the values of sin $^{2}$2 θ$_{13}$ = 10 − $^{2}$, 10 − $^{3}$, 10 − 4 and 10 − 5 from top to bottom. In the case of sin $^{2}$2 θ$_{13}$ = 10 − 2 and 10 − $^{3}$, P ( E$_{ν}$ ) and ¯ P ( E$_{ν}$ ) are about 0 when shock wave does not reach H-resonance ( t = 0 − 2 s). However, in later time ( t = 2 − 5 s), P ( E$_{ν}$ ) and ¯ P ( E$_{ν}$ ) become finite. These effects appear from low-energy side and gradually shift toward high-energy side as the time passes by. In the case of sin $^{2}$2 θ$_{13}$ = 10 − $^{5}$, P ( E$_{ν}$ ) and ¯ P ( E$_{ν}$ ) hardly change with time, and are about 0.3 and III. RESULT AND DISCUSSIONS A. Survival probability 10