Ultrarelativistic ideal Fermi gas
= Ultrarelativistic ideal Fermi gas
For spin-one-half particles in three dimensions with dispersion $\varepsilon=pc$, the <density of states> is
$$
g(\varepsilon)=\frac{V\varepsilon^2}{\pi^2\hbar^3c^3}.
$$
At zero temperature,
$$
E_F=\hbar c\left(3\pi^2\frac NV\right)^{1/3},
\qquad
E=\frac34NE_F,
\qquad
p=\frac E{3V}.
$$