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[^4]: From the numerical simulations we find that the variations of the numerical results for the order parameter, $delta S$ and $delta A$, are rather small, so that the approximation $delta S=delta Asimeqdelta S_{infty}$ may be adopted without approximation.
[^5]: The negative sign of $Gamma_{etau}$ (cf. Eq.([g1])) would lead to the more complicated form of the CP asymmetry in the active-sterile neutrino oscillations.
[^6]: For $delta m^2ll m^2$, Eq.([ms]) can be expanded as $|U_{e2}|^2=1-(2/3)delta m^2/m^2$.
[^7]: In the case of $mu$- or $tau$-flavor oscillation, the amplitude $|a|$ is much smaller than unity, and we can ignore the term $2(omega-delta m^2/2|a|)$ in the integrand of Eq.([delms]).
[^8]: Similar sensitivities to $sin^2 2theta_{rm sun}$ and $delta m^2$ are also found for solar $
u_e$ and $overline{
u}_e$ oscillations in the full 3-generation mixing case (i.e. without $mu$- and $tau$-flavor oscillation). The case for the CP asymmetry in the active-sterile neutrino oscillations has been studied in detail in Ref.[@brupp].
[^9]: It is possible that $Gamma_{etau}$ is negative
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