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Etudes des proprietes des neutrinos dans les contextes ...

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

Luminosity (a.u.)<br />

1e+13<br />

8e+12<br />

6e+12<br />

4e+12<br />

2e+12<br />

0 20 40 60 80<br />

Neutrino Energy (MeV)<br />

Figure 3.3: Neutrino fluxes at the <strong>neutrinos</strong>phere: the curves show the Fermi-<br />

Dirac distributions used for electron <strong>neutrinos</strong> with Tνe= 3.2 MeV (solid), electron<br />

anti-<strong>neutrinos</strong> T¯νe= 4.8 MeV (dashed) and for the other flavors Tνx= 7.6<br />

MeV (with νx = νµ, ντ, ¯νµ, ¯ντ) (dotted line).<br />

Reaction Rates<br />

As seen earlier, the dominant reactions that control the n/p ratio is the capture<br />

reactions on free nucleons<br />

νe + n ⇋ p + e − , (3.24)<br />

and<br />

¯νe + p ⇋ n + e + . (3.25)<br />

In our calculation [26] (see chapter 5) we took a simplified formula 9 for the<br />

reaction cross sections, namely [100]<br />

and<br />

σνe(Eνe) ≈ 9.6 × 10 −44<br />

σ ¯νe(E ¯νe) ≈ 9.6 × 10 −44<br />

2 Eνe + ∆np<br />

cm<br />

MeV<br />

2 , (3.26)<br />

2 E¯νe − ∆np<br />

cm<br />

MeV<br />

2 , (3.27)<br />

where ∆np ≈ 1.293 MeV is the neutron proton mass difference. The associated<br />

rates can be written as [67]<br />

<br />

dLν<br />

λ = σ(E)ν dEν. (3.28)<br />

dEν<br />

9 Such cross sections can also be computed numerically exactly. For simplicity we ignored<br />

weak magnetism and recoil corrections, which may be important [76].<br />

61

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