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Fractional quantized vortices as direct evidence of d_x^2^_-_y^2^_-wave pairing symmetry up to critical temperature in high-Tc cuprate superconductors

家成 井口, Ienari Iguchi

Published Jan 1, 2002• 0 citations
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A recent Bose–Einstein condensation (BEC) model of several cuprate superconductors is based on bosonic Cooper pairs (CPs) moving in 3D with a quadratic energy-momentum (dispersion) relation. The 3D BEC condensate-fraction versus temperature formula poorly fits penetration-depth data for two cuprates in the range 1/2<T/Tc≤1 where Tc is the BEC transition temperature. We show how these fits are dramatically improved, assuming cuprates to be quasi-2D, and how equally good fits are obtained for conventional 3D and quasi-1D nanotube superconducting data, provided the correct linear CP dispersion is assumed in BEC at their assumed corresponding dimensionalities. This is offered as additional concrete empirical evidence for linearly-dispersive pairs in another recent BEC scenario of superconductors within which a BCS condensate turns out to be a very special case.
The phase diagram of hole-doped cuprate superconductors contains three central puzzles: a dome-shaped superconducting phase, a strange metal normal state with Planckian dissipation, and robust d-wave pairing (dx2-y2 symmetry). We propose a unified framework based on a single material-dependent parameter, the coherence purity p, which measures the fraction of phase-coherent condensate relative to dissipative channels. Geometric frustration of the antiferromagnetic background on the CuO2 square lattice drives p to a maximum at optimal doping. The superconducting transition temperature follows T_c proportional to p/(1-p). The d-wave symmetry is derived as the leading pairing instability under on-site repulsion and nearest-neighbor superexchange, without being assumed. In the strange metal, the Planckian dissipation coefficient alpha = hbar/(tau kB T) is linked to the purity deficit 1-p through a universal amplification factor C ≈ 31, which we derive from the nodal Dirac structure of the d-wave state. Fitting the superconducting domes of LSCO and YBCO with the peak purity p_max = 0.97 (fixed from independent transport and high-energy experiments) yields excellent agreement using only two material-dependent scale parameters. The framework produces falsifiable predictions for the doping dependence of the superfluid density and for the product of maximum T_c and the Planckian coefficient. Keywords: high-temperature superconductivity, cuprates, strange metal, Planckian dissipation, d-wave pairing, coherence purity, superconducting dome, LSCO, YBCO