Abstract

We propose a model for high-Tc_{c} superconductors, valid for 0δδSC0\leq\delta\leq\delta_{SC}, that includes both the spin fluctuations of the Cu++^{++} magnetic ions and of the O^{--} doped holes. Spin-charge separation is taken into account with the charge of the doped holes being associated to quantum skyrmion excitations (holons) of the Cu++^{++} spin background. The holon effective interaction potential is evaluated as a function of doping, indicating that Cooper pair formation is determined by the competition between the spin fluctuations of the Cu++^{++} background and of spins of the O^{--} doped holes (spinons). The superconducting transition occurs when the spinon fluctuations dominate, thereby reversing the sign of the interaction. At this point (δ=δSC\delta = \delta_{SC}), the theory is supersymmetric at short distances and, as a consequence, the leading order results are not modified by radiative corrections. The critical doping parameter for the onset of superconductivity at T=0 is obtained and found to be a universal constant determined by the shape of the Fermi surface. Our theoretical values for δSC\delta_{SC} are in good agreement with the experiment for both LSCO and YBCO.Comment: RevTex, 4 pages, no figure

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