\[\newcommand{\bra}[1]{\langle#1|} \newcommand{\ket}[1]{|#1\rangle} \newcommand{\braket}[2]{ \langle #1 | #2 \rangle}\]

Fermi gas

Now we should get back to the ideal gas but treating particles as quantum fermions.

\[\epsilon_k = \frac{k^2}{2m}\] \[P_{dg}= \frac{2\hbar^2}{m_e}\left(\frac{Z}{A}\right)^{5/3}\left(\frac{\rho}{m_p}\right)^{5/3}\]