Fig. 4: Specific heat away from the nematic QCP(δ ≠ 0).
From: Unconventional superconductivity near a nematic instability in a multi-orbital system
We plot the variation of the specific heat coefficient scaled by the density of state on Fermi surface, N0 with the reduced temperature T/Tc for a set of values of the nematic mass δ = 0.01 and 0.1. Here, Tc is the superconducting transition temperature. The black dashed line represents the normal state contribution and is equal to 2π2/3. There is a finite specific heat jump at the transition point represented by the vertical line for both values of δ.
