text: This clearly aﬀects nk because it is expressed via the full 
  Green’s function and competes with the conventional ef- 
  fect of the gap opening. The distribution function from 
  this model, which we show in Fig.2b brings this point 
  out by showing that in a MFLI model, at ǫ < 0, nk in a 
  superconductor is larger than nk in the normal state, in 
  clear diﬀerence with the BCSI case. 
  
  We analyzed the original MFLI model for various pa- 
  rameters and found that the behavior presented in Fig. 
  12, where ∆W (ωc) > 0 for all frequencies, is typical but 