Electronic heat capacity of a heavy Fermi liquid
= Electronic heat capacity of a heavy Fermi liquid
For <quasiparticles> with <density of states> $g(E_F)$ including both spins, the leading <electronic heat capacity> is $C=\gamma T$ with $\gamma=\pi^2k_B^2g(E_F)/3$. A narrow heavy band makes this coefficient large. The <density of states> and heat capacity must use consistent extensive, molar or volumetric normalization.