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Etudes des proprietes des neutrinos dans les contextes ...

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tel-00450051, version 1 - 25 Jan 2010<br />

This last formula prove that the function fe is not the constant zero function<br />

Aee = Bee and consequently:<br />

P(νe → νe, δ = 0) = P(νe → νe, δ = 0) (4.75)<br />

Therefore , when δ is taken non zero, it has an influence on the value of P(νe →<br />

νe, δ). The νe and ¯νe fluxes will depend on δ even when the luminosities Lνµ and<br />

Lντ are taken equal at the neutrino-sphere:<br />

φνe(δ) = LνeP(νe → νe, δ) + Lνµ (P(νµ → νe) + P(ντ → νe))<br />

= LνeP(νe → νe, δ) + Lνµ (1 − P(νe → νe, δ))<br />

= (Lνe − Lνµ)P(νe → νe, δ) + Lνµ<br />

(4.76)<br />

This analytical derivation proving that, if the dependence on δ of the evolution<br />

operator cannot be factorized then the electron neutrino survival probability depends<br />

on δ, is the first to be performed. Neverthe<strong>les</strong>s, this implication had been<br />

observed numerically. We can easily generalize this derivation which implies that<br />

as soon as the medium effect on νµ and on ντ is not the same, effects of the CPviolating<br />

phase on the electron neutrino (and anti-neutrino) fluxes will appear.<br />

88

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