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Etudes des proprietes des neutrinos dans les contextes ...

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

Figure 5.4: Total νe survival probability as a function of time, where τ ≡<br />

(∆m 2 /2p0)t and p0 ≃ 2.2 T. The curves are for different values κ of the neutrino<br />

self-coupling as indicated where κ = 0 corresponds to vacuum oscillations.<br />

Figure 5.5: Evolution of the νe survival probability for three values of the neutrino<br />

momenta in the presence of a strong neutrino self-potential term (κ = 10).<br />

Fig.(5.4). But when κ is fixed to a high value, which means the self-interactions<br />

are important, then even from three different values of momentum, the oscillations<br />

are pretty much synchronized as one can see on Fig.(5.5) This behaviour<br />

can happen in the Early Universe or in core-collapse supernova. In the latter<br />

environment there is matter and the density of <strong>neutrinos</strong> is decreasing with time.<br />

This implies the possible presence of a bipolar regime.<br />

5.2.2 The bipolar regime<br />

Neutrino-neutrino interaction can lead to collective flavor conversion effects in<br />

supernovae when bipolar oscillations occur, even when the mixing angle is very<br />

small, contrary to the usual MSW effect. Such behaviour can be interpreted as a<br />

pendulum in flavour space, using the polarization vector formalism. We first show<br />

the possibility to <strong>des</strong>cribe the system as an oscillating pendulum in the simp<strong>les</strong>t<br />

98

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