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Stars as Laboratories for Fundamental Physics - MPP Theory Group

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468 Chapter 12<br />

Fig. 12.8. Lower limit on τ γ /m ν <strong>for</strong> m ν ∼<br />

< 40 eV and τtot /m ν ∼<br />

> 5×10 5 s/eV<br />

(most neutrinos p<strong>as</strong>s the Earth be<strong>for</strong>e decaying).<br />

Fig. 12.9. Upper limit on the radiative branching ratio B γ <strong>for</strong> m ν ∼<br />

< 40 eV<br />

and τ tot /m ν ∼<br />

< 5×10 5 s/eV (most neutrinos decay between SN 1987A and<br />

Earth).<br />

shown in Fig. 12.9. The most conservative c<strong>as</strong>e yields approximately<br />

B γ < 3×10 −10 . As a bound on an effective transition moment this is<br />

µ eff < 0.7×10 −5 µ B m −2<br />

eV (m eV /τ s ) 1/2 , (12.19)<br />

where τ s = τ tot /s. Of course, if τ tot became so short that the neutrinos<br />

would decay while still within the envelope of the progenitor even this

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