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Etudes des proprietes des neutrinos dans les contextes ...

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

Chapter 5<br />

Neutrino-neutrino interactions<br />

The neutrino-neutrino interactions induce a new paradigm in neutrino physics.<br />

When a medium is teeming with <strong>neutrinos</strong>, such as the early Universe or during<br />

a Supernova explosion, <strong>neutrinos</strong> can interact with each other in addition with<br />

the matter present. When the density of <strong>neutrinos</strong> reach a certain value, the<br />

self interaction can even become dominant in comparison with other interactions<br />

such as with matter. Such interactions create new effects, that turn out to be<br />

collective. These new phenomena have attracted the interest of the world wide<br />

community working on neutrino astrophysics [[105, 101, 108, 64, 44, 62, 101, 32,<br />

24, 64, 95, 61, 54, 72, 104, 103, 42, 51, 94, 53, 52, 55, 59, 60, 58, 69]]. After a<br />

few years of very fast developments, a new picture of neutrino propagation has<br />

emerged, we <strong>des</strong>cribe here the present status. However, we might still be far from<br />

a definite comprehension since new ideas and interpretations keep being proposed.<br />

Here we present the current understanding of these collective phenomena. They<br />

depend on the hierarchy, and can be classified as follows: first a synchronization<br />

stage which can occur both in the early Universe environment and in supernovae,<br />

second, bipolar resonances and spectral splits that take place in the supernova<br />

environment. Let us explain when and why such phenomena emerge.<br />

5.1 Theoretical framework<br />

5.1.1 The effective interaction Hamiltonian<br />

We start with the derivation of the effective Hamiltonian which is done just<br />

like the one for the interaction with matter. Neutrinos will interact with other<br />

<strong>neutrinos</strong> via the neutral current interaction. For neutrino energies much <strong>les</strong>s<br />

than the mass of the Z 0 boson, the effective interaction is<br />

H NC<br />

ν−ν = GF<br />

√2<br />

<br />

α=e,µ,τ<br />

¯ναLγ µ (1 − γ5)ναL<br />

89<br />

<br />

β=e,µ,τ<br />

¯νβLγµ(1 − γ5)νβL<br />

<br />

. (5.1)

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