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Stars as Laboratories for Fundamental Physics - MPP Theory Group

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Chapter 9<br />

Oscillations<br />

of Trapped Neutrinos<br />

In a supernova (SN) core or in the early universe neutrinos scatter on<br />

the background medium and on each other. There<strong>for</strong>e, oscillations of<br />

mixed neutrinos are frequently interrupted, leading to flavor equilibrium<br />

if there is enough time. A Boltzmann-type kinetic equation is<br />

derived that accounts simultaneously <strong>for</strong> neutrino oscillations and collisions<br />

<strong>for</strong> arbitrary neutrino degeneracy. It is applied to a SN core,<br />

yielding an estimate of the time scale to reach flavor equilibrium. On<br />

the b<strong>as</strong>is of the SN 1987A neutrino observations a limit on the mixing<br />

of sequential neutrinos with a hypothetical sterile flavor is derived.<br />

9.1 Introduction<br />

So far oscillations were discussed in the context of “beam experiments”<br />

where neutrinos of a known flavor are produced at a certain location,<br />

<strong>for</strong> example in a power reactor or in the Sun, then propagate over a<br />

distance, and are then detected with a device that allows one to distinguish<br />

between different flavors. It w<strong>as</strong> <strong>as</strong>sumed that there were no<br />

interactions between the production and detection point, with the possible<br />

exception of decays, allowing one to treat neutrino oscillations <strong>as</strong><br />

a simple propagation phenomenon fully analogous to light propagation<br />

in an optically active medium.<br />

This approach is not adequate <strong>for</strong> the early universe and a young SN<br />

core. In both c<strong>as</strong>es there are frequent neutrino collisions which affect<br />

the free evolution of the ph<strong>as</strong>es. The impact of these collisions can<br />

be understood if one <strong>as</strong>sumes <strong>for</strong> the purpose of illustration that one<br />

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