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Etudes des proprietes des neutrinos dans les contextes ...

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

trinos of all flavors are produced in the hot core of the proto-neutron star, which<br />

has a temperature of about 40 MeV, through electron-positron pair annihilation,<br />

electron-nucleon bremsstrahlung,<br />

nucleon-nucleon bremsstrahlung,<br />

plasmon decay<br />

and photo-annihilation<br />

e + + e − → νl + νl, (3.9)<br />

e ± + N → e ± + N + νl + νl, (3.10)<br />

N + N → N + N + νl + νl, (3.11)<br />

γ → νl + νl, (3.12)<br />

γ + e ± → e ± + νl + νl, (3.13)<br />

Electron <strong>neutrinos</strong> are also produced by the electron capture process in Eq.(3.3),<br />

and electron anti<strong>neutrinos</strong> are produced by positron capture on neutrons. Even<br />

though the <strong>neutrinos</strong> interact weakly with matter, they are trapped in the SN<br />

core because of the very high matter density. When the matter density is low<br />

enough (of the order of 10 11 g.cm −3 ), <strong>neutrinos</strong> can exit freely of the mantle of<br />

the proto-neutron star since their mean free path is larger than the radius of the<br />

core. The sphere from which <strong>neutrinos</strong> stream out freely is called the neutrino<br />

sphere.<br />

The neutrino spheres<br />

The neutrino energy being too low in such environments to create muons and<br />

taus by charged-current, the medium is only composed of protons, neutrons,<br />

and electrons. This implies the existence of different energy dependent neutrino<br />

spheres for different neutrino flavors whose estimated radii are typically between<br />

50 and 100 km. There are roughly three energy-dependent neutrino spheres: one<br />

for νe, one for νe and one for νµ, νµ, ντ, ντ. Indeed, the flavor <strong>neutrinos</strong> νe and νe<br />

can interact with the medium through both charged-current and neutral-current<br />

weak processes, whereas the <strong>neutrinos</strong> νµ, νµ, ντ, ντ can interact only through<br />

neutral current weak processes, which are flavor-independent. From now on, in<br />

this chapter, we will denote νµ, νµ, ντ, ντ collectively as νx, as usually done in the<br />

literature. After the shock breakout, each neutrino sphere produces a thermal<br />

flux of the corresponding neutrino flavor. In the next section, we will give a model<br />

of these thermal fluxes.<br />

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