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Stars as Laboratories for Fundamental Physics - MPP Theory Group

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xx<br />

Preface<br />

scales that have been used <strong>for</strong> the purposes of particle <strong>as</strong>trophysics.<br />

For each c<strong>as</strong>e the salient applications are summarized. Chapters 3−6<br />

deal with the interaction of “radiation” (neutrinos, axions, other lowm<strong>as</strong>s<br />

bosons) with the main constituents of stellar pl<strong>as</strong>m<strong>as</strong> (photons,<br />

electrons, nucleons). In these chapters all in<strong>for</strong>mation is pulled together<br />

that pertains to the given interaction channel, even if it is not directly<br />

related to the energy-loss argument. For example, in Chapter 5 the<br />

limits on the electromagnetic coupling of pseudoscalars with photons<br />

are summarized; the stellar energy-loss ones are the most restrictive<br />

which justifies this arrangement.<br />

Chapter 6 develops the topic of particle dispersion in media. The<br />

medium-induced photon dispersion relation allows <strong>for</strong> the pl<strong>as</strong>ma process<br />

γ → νν which yields the best limit on neutrino dipole moments<br />

by virtue of the energy-loss argument applied to globular-cluster stars.<br />

The neutrino dispersion relation is needed <strong>for</strong> the following discussion<br />

of neutrino oscillations, establishing a link between the energy-loss argument<br />

and the dispersion arguments of the following chapters.<br />

Dispersion and propagation effects are particularly important <strong>for</strong><br />

m<strong>as</strong>sive neutrinos with flavor mixing. To this end the phenomenology<br />

of m<strong>as</strong>sive, mixed neutrinos is introduced in Chapter 7. Vacuum and<br />

matter-induced flavor oscillations <strong>as</strong> well <strong>as</strong> magnetically induced spin<br />

oscillations are taken up in Chapter 8. If neutrinos are in thermal equilibrium<br />

<strong>as</strong> in a young SN core or the early universe, neutrino oscillations<br />

require a different theoretical treatment (Chapter 9).<br />

Chapters 10−13 are devoted to <strong>as</strong>trophysical sources where neutrinos<br />

have been me<strong>as</strong>ured, i.e. the Sun and supernovae (<strong>for</strong> the latter<br />

only the SN 1987A signal exists). Neutrino oscillations, notably<br />

of the matter-induced variety, play a prominent role in Chapter 10<br />

(solar neutrinos) and Chapter 11 (SN neutrinos). Radiative particle<br />

decays, especially of neutrinos, are studied in Chapter 12 where the<br />

Sun and SN 1987A figure prominently <strong>as</strong> sources. In Chapter 13 the<br />

particle-physics results from SN 1987A are summarized, including the<br />

ones related to the energy-loss and other arguments.<br />

Chapters 14−16 give particle-specific summaries. While axions play<br />

a big role throughout this text, only the structure of the interaction<br />

Hamiltonian with photons, electrons, and nucleons is needed. Thus<br />

everything said about axions applies to any pseudoscalar low-m<strong>as</strong>s boson<br />

<strong>for</strong> which they serve <strong>as</strong> a generic example. In Chapter 14 these<br />

results are interpreted in terms of axion-specific models which relate<br />

their properties to those of the neutral pion and thus establish a nearly<br />

unique relationship between their m<strong>as</strong>s and interaction strength. Often-

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