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It is shown that the main features of the phase diagram for high Tc superconductivity can be calculated as a function of doping in a simple, essentially unique non-Landau/Fermi liquid with quartic interactions.
- The phase diagram depends on a single parameter 0<gamma<1 determined by the strength of the interaction at short distances.
- A new d-wave gap equation has solutions that fall under a superconducting dome, which terminates at the renormalization group fixed point.
- Optimal doping is estimated to occur just below 3/2 \pi^2.
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