Abstract
The precursor non-superconducting pairing of carriers and the novel superconductivity in high- T c cuprates are studied within the large (bi)polaron model and the new BCS-like fermion and boson mean-field approximations by treating a two-component charge carrier picture. It is argued that pre-formed pairs (large bipolarons) reside in underdoped cuprates between the CuO 2 planes and remain localized in the z-direction. With lowering temperature, these large bipolarons condense into a superfluid quasi-one-dimensional Bose-liquid state. In the intermediate electron–phonon coupling regime, the Cooper-pair formation and condensation in the CuO 2 layers occur also at different temperatures. Large bipolarons and polaron Cooper pairs in optimally doped cuprates condense into a superfluid Bose-liquid state almost at the same temperature due to the doping-induced dimensional crossover.
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