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Stars as Laboratories for Fundamental Physics - MPP Theory Group

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Radiative Particle Decays 459<br />

Fig. 12.4. Spectrum of photons from the solar neutrino decay ν e → ν ′ γ <strong>for</strong><br />

the indicated values of the anisotropy parameter α. Me<strong>as</strong>urements of the<br />

x-ray emission of the solar corona (open diamonds) according to Chodil et<br />

al. (1965). Upper limit x- and γ-ray fluxes according to Frost et al. (1966)<br />

and Peterson et al. (1966). Estimated albedo according to Peterson et al.<br />

(1966). Thin solid line: Maximally allowed photon spectrum from neutrino<br />

decay. (Figure adapted from Raffelt 1985.)<br />

With Eq. (7.12) this translates into<br />

µ eff < 5×10 −6 µ B m −2<br />

eV . (12.10)<br />

It must be stressed, again, that the recent progress in solar neutrino<br />

<strong>as</strong>tronomy h<strong>as</strong> placed this result on the same footing <strong>as</strong> a terrestrial<br />

experiment—the magnitude of the solar neutrino flux and its main<br />

spectral features are now experimentally established!

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