“…Such observables include: the critical SC transition temperature as a function of doping, T c (x), the pseudogap transition temperature as a function of doping, T * (x), the pressure dependence of the optimal SC transition temperature T max (P), the dependence of the optimal SC transition temperature on the number of CuO 2 layers, T max (N ), the resistivity as a function of temperature and magnetic field (ρ(T ) and ρ(H)) in the normal (non SC) phases and the spectral weight, among other observable quantities. All of these compare quite well with the experimental data for several cuprate materials [1][2][3][4] including LSCO, YBCO, Hg1201, Hg1212, Hg1223, Bi2201, Bi2212, Bi2213. Our theory is, therefore, testable and thus fulfills one of the first pre-requisites of any acceptable theory and, beyond that, it has proven to pass all the tests to which it has been submitted so far.…”