The Hidden Fermi liquid theory

This week I have been re-reading Phil Anderson's paper,  The `strange metal' is a Fermi liquid with edge singularities. Here is a brief summary of some of the main things I gleaned from the paper. The question is:
What is the nature of the excitations (and one-electron Greens function) of the Hubbard model in the infinite-U limit and for large dopings (perhaps x greater than 0.3) above which superconductivity occurs?
Anderson claims:

• the strong interactions lead to a significant particle-hole asymmetry [which should be visible in tunneling spectra] 
• excitations exhibit anomalous forward scattering
• the quasi-particle weight Z vanishes on the Fermi surface

• there is  a formal similarity of this problem with that of Fermi-edge singularities in the X-ray spectra of metals, where the one-electron Greens function has a power law decay associated with the phase shift from an infinite potential.

• A simple argument (exploiting the Friedel sum rule) gives the main quantitative prediction of the theory a value for the doping (x) dependence of the exponent

• a power-law frequency dependence of the optical conductivity
• this theory may have some similarities to one of Norman and Chubukov.
• Quasiparticles emerge in the superconducting and pseudogap states: "But above T* and above the gap energy the quasiparticles experience power-law decay: essentially, the line of quasiparticle poles turns into a cut in the complex  plane."