28.01.2015 Views

Stars as Laboratories for Fundamental Physics - MPP Theory Group

Stars as Laboratories for Fundamental Physics - MPP Theory Group

Stars as Laboratories for Fundamental Physics - MPP Theory Group

SHOW MORE
SHOW LESS

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

Chapter 6<br />

Particle Dispersion and<br />

Decays in Media<br />

Dispersion effects in media have a significant impact on the propagation<br />

of some low-m<strong>as</strong>s particles (photons, neutrinos) while others are<br />

left unaffected (axions and other Nambu-Goldstone bosons). The relationship<br />

between <strong>for</strong>ward scattering and refraction is derived, and the<br />

dispersion relations <strong>for</strong> photons and neutrinos are thoroughly studied.<br />

Modified particle dispersion relations allow certain decay processes to<br />

occur in media that cannot occur in vacuum, notably the photon decay<br />

γ → νν which dominates the neutrino emissivity in a wide range<br />

of temperatures and densities (“pl<strong>as</strong>ma process”). Other examples are<br />

the neutrino and majoron decay ν → νχ and χ → νν, respectively.<br />

The rates <strong>for</strong> such processes are derived. The pl<strong>as</strong>ma process allows<br />

one to derive the most restrictive limits on neutrino magnetic dipole<br />

moments. Screening effects in reactions involving Coulomb scattering,<br />

and neutrino electromagnetic <strong>for</strong>m factors in media are discussed.<br />

6.1 Introduction<br />

Particles are the quantized excitations of certain fields—photons of the<br />

electromagnetic field, electrons of the electron field, and so <strong>for</strong>th. It<br />

is usually convenient to expand these fields in plane waves characterized<br />

by frequencies ω and wave vectors k; the excitations of these modes<br />

then exhibit a temporal and spatial behavior proportional to e −i(ωt−k·x) .<br />

The frequency <strong>for</strong> a given wave number is determined by the dispersion<br />

relation. Because (ω, k) is a four-vector, and because of Lorentz<br />

invariance, in vacuum the quantity ω 2 − k 2 = m 2 is the same <strong>for</strong> all<br />

193

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!