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Etudes des proprietes des neutrinos dans les contextes ...

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

Flux ratio<br />

Flux ratio<br />

1.1<br />

1<br />

0.9<br />

0 10 20 30 40 50 60 70<br />

Energy (MeV)<br />

Figure 6.2: Ratios of the νe fluxes for a CP violating phase δ = 180 ◦ over δ = 0 ◦ as<br />

a function of neutrino energy, at 1000 km within the star. The curves correspond<br />

to the following cases : Hνν = 0 and Vµτ = 0 (dotted), Hνν = 0 and Vµτ = 0<br />

(dashed) and Hνν = 0 and Vµτ = 0 (solid). These are obtained with Lνµ = Lντ<br />

e.g. Tνµ = 1.05 Tντ. The case Hνν = 0 and Vµτ = 0 (dot-dashed) with Lνµ = Lντ<br />

is also shown. The results correspond to an inverted hierarchy and a small θ13.<br />

1.05<br />

1<br />

0.95<br />

0 10 20 30 40 50<br />

Energy (MeV)<br />

Flux ratio<br />

1.05<br />

1<br />

0.95<br />

0 25 50 75 100 125<br />

Energy (MeV)<br />

Figure 6.3: Ratios of the νe fluxes for a CP violating phase δ = 180 ◦ over δ = 0 ◦<br />

as a function of neutrino energy. They correspond to inverted hierarchy and small<br />

θ13 and different distances from the neutron star surface, i.e. 200 km (dotted),<br />

500 km (dashed), 750 (dot-dashed), 1000 (solid). The results include the ν-ν<br />

interaction and the Vµτ refractive index. They are obtained using equal νµ and<br />

ντ fluxes at the <strong>neutrinos</strong>phere (left) or taking Tνµ = 1.05 Tντ (right). For the ¯νe<br />

fluxes deviations up to 10% are found at energies lower than 10 MeV.<br />

119

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