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Etudes des proprietes des neutrinos dans les contextes ...

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

x<br />

B<br />

2 ˜ θV<br />

z<br />

P<br />

¯P<br />

D<br />

y<br />

Figure 5.8: Left figure: schematic view of the initial condition of the system.<br />

Right: schematic picture of the evolution. Black ellipse represents the precession<br />

of P and ¯ P around the Hamiltonian. Black wigg<strong>les</strong> represent the nutation created<br />

by the vector D. Violet arc represents the diminution of µ which in addition to<br />

the variations of D will lead to a global simultaneous decrease of Pz, ¯Pz and Dz<br />

may extend Pω to negative frequencies such that ¯ Pω = P−ω (ω > 0) and use<br />

only Pω with −∞ < ω < +∞. In these terms, D = +∞<br />

−∞ dω sω Pω, where sω ≡<br />

sign(ω) = ω/|ω|. To comprehend analytically the spectral split phenomenon, we<br />

have to use several approximations. To do so, let us state first that we work in<br />

the flavour basis. In this basis we have for the vacuum term10 :<br />

⎛ ⎞<br />

and for the matter term:<br />

B = ⎝<br />

sin 2 ˜ θV<br />

0<br />

cos 2 ˜ θV<br />

⎛<br />

λL = ⎝<br />

0<br />

0<br />

λ<br />

⎞<br />

x<br />

¯P<br />

H<br />

z<br />

P<br />

⎠ . (5.50)<br />

⎠ . (5.51)<br />

10 We use the relation ˜ θV = π/2 − θV with θV is the vacuum mixing angle, having ˜ θV close<br />

to π/2 means we work in the inverted hierarchy.<br />

105<br />

y

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