01.05.2013 Views

Etudes des proprietes des neutrinos dans les contextes ...

Etudes des proprietes des neutrinos dans les contextes ...

Etudes des proprietes des neutrinos dans les contextes ...

SHOW MORE
SHOW LESS

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

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

P(ν e →ν e )<br />

1<br />

0.8<br />

0.6<br />

0.4<br />

0.2<br />

0<br />

0 20 40 60<br />

E [MeV]<br />

Figure 7.3: Electron anti-neutrino probabilities at the edge of 1D core-collapse<br />

supernova at t =2 s. Phase effects are apparent as fast changes as a function of<br />

neutrino energies.<br />

few percent modification can appear due to the presence of Vµτ and of non-linear<br />

effects [69] (see chapter 6). One of the important open questions is the hierarchy,<br />

can be positive (normal) or negative (inverted hierarchy).<br />

since the sign of ∆m2 23<br />

The value of the third neutrino mixing angle is another issue, particularly crucial<br />

for the search of CP violation in the lepton sector. We take here two possible<br />

values for θ13, a large (sin2θ13 = 10−4 ) and a small (sin2θ13 = 10−8 ). Note that<br />

the results corresponding to the large value are emblematic of the whole range<br />

sin2θ13 > 10−4 up to the present experimental Chooz limit. They correspond<br />

to the case of the adiabatic conversion at the high density resonance [86]. The<br />

other value is chosen as an example of the non-adiabatic regime. Note that<br />

sin22θ13 = 10−4 − 10−5 are the smal<strong>les</strong>t values that can be reached in accelerator<br />

experiments even with long-term projects such as super-beams, beta-beams or<br />

neutrino factories [115]. As we will argue, the positron time signal produced by<br />

charged-current events presents specific features depending on the hierarchy and<br />

on θ13 since this affects the neutrino flavor conversions at the MSW high resonance<br />

region.<br />

For the neutrino luminosities at the neutrino-sphere we make the usual assumption<br />

of equipartition of energies among all neutrino flavors and that they<br />

decrease exponentially with time Lν = Lν0 × exp(−t/τ) with Lν0 = 1052 erg ·<br />

s−1 and τ = 3.5 s. Equal luminosities are appropriate for the cooling phase of<br />

the neutrino signal upon which we are focusing; during the accretion phase the<br />

νe and ¯νe luminosities are substantially brighter than the νx [84]. The average<br />

energies of each neutrino flavor follows a hierarchy i.e. 〈Eνe〉 < 〈E¯νe〉 < 〈Eνx〉<br />

with typical values of 12, 15 and 18 MeV respectively.<br />

127

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!