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.

600 Appendix D<br />

D.2 Nuclear Matter<br />

D.2.1<br />

The Ideal p n e ν e G<strong>as</strong><br />

For the topics discussed in this book, the properties of hot nuclear<br />

matter in a young supernova core are of great interest. The relevant<br />

range of densities and temperatures is about 3×10 12 −3×10 15 g cm −3<br />

and 3−100 MeV, respectively. The properties of matter at such conditions<br />

is determined by its equation of state which takes the nuclear<br />

interaction fully into account. However, in order to gain a rough understanding<br />

of the behavior of the main constituents of the medium<br />

(protons, neutrons, electrons, and electron neutrinos) it is worthwhile<br />

to study a simple toy model where these particles are treated <strong>as</strong> ideal<br />

Fermi g<strong>as</strong>es.<br />

To this end, neutrinos and electrons are treated <strong>as</strong> m<strong>as</strong>sless. Their<br />

dispersion relation is dominated by the interaction with the medium.<br />

Because they interact only by electroweak <strong>for</strong>ces their “effective m<strong>as</strong>s”<br />

is always much smaller than their energies.<br />

D.2.2<br />

Kinetic and Chemical Equilibrium<br />

The reaction e p ↔ n ν e which establishes β equilibrium is f<strong>as</strong>t compared<br />

to other relevant time scales. There<strong>for</strong>e, the relative abundances<br />

of n, p, e, and ν e are determined by the conditions of kinetic and chemical<br />

equilibrium. The physical condition of the medium is then determined<br />

by the baryon density n B , the temperature T , and the condition<br />

of electric charge neutrality<br />

n B = n n + n p Baryon density,<br />

n p = n e Charge neutrality, (D.18)<br />

µ e + µ p = µ n + µ νe β equilibrium.<br />

Here, the µ j are the relativistic chemical potentials of the fermions<br />

which determine their number densities n j according to the Fermi-Dirac<br />

distribution Eq. (D.5). Recall that n j is the difference between fermions<br />

and antifermions of a given species.<br />

In addition, one of two extreme <strong>as</strong>sumptions is made. In a young<br />

SN core the neutrinos are trapped so that the local lepton number is<br />

conserved. In this c<strong>as</strong>e the lepton fraction Y L is the fourth required<br />

input parameter,<br />

Y L n B = n e + n νe Lepton conservation. (D.19)

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

Saved successfully!

Ooh no, something went wrong!