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Phase diagram and dependence of the critical temperature T_c on the pressure for Tl_{0.5}Pb_{0.5}Sr_2Ca_{1-x}Y_xCu_2)_7
Using a mean-field BCS-like approach on the bidimensional extended Hubbard
Hamiltonian we calculate the superconducting transition temperature Tc as a
function of the hole content nh, for the d-wave and extended-s wave gap
symmetries. To describe the pressure effect on Tc we assume it induces a change
in the magnitude V of the attractive superconductor potential. This assumption
yields an explanation for the intrinsic term, and together with the well known
change in nh, we set the critical temperature as Tc=Tc(nh(P),V(P)). With this
we obtain a general expansion of Tc in terms of the pressure P and the hole
content nh. We apply this expansion to the
Tl_{0.5}Pb_{0.5}Sr_2Ca_{1-x}Y_xCu_2)_7 system
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