A Theoretical Approach to Pseudogap and Superconducting Transitions in Hole-Doped Cuprates
Figure 7
A plot of the electron and hole reciprocal QPLT as a function of weak disorder potential using (30) for . The former is assumed to be centered at and whereas the latter at of the first Brillouin zone. One notices that the former is short-lived compared to the latter for very weak to moderately weak disorder potential.
