Fermi-surface transformation across the pseudogap critical point of the cuprate superconductor LaNdSrCuO
arXiv:1607.05693 · doi:10.1103/PhysRevB.95.224517
Abstract
The electrical resistivity and Hall coefficient R of the tetragonal single-layer cuprate Nd-LSCO were measured in magnetic fields up to T, large enough to access the normal state at , for closely spaced dopings across the pseudogap critical point at . Below , both coefficients exhibit an upturn at low temperature, which gets more pronounced with decreasing . Taken together, these upturns show that the normal-state carrier density at drops upon entering the pseudogap phase. Quantitatively, it goes from at to at . By contrast, the mobility does not change appreciably, as revealed by the magneto-resistance. The transition has a width in doping and some internal structure, whereby R responds more slowly than to the opening of the pseudogap. We attribute this difference to a Fermi surface that supports both hole-like and electron-like carriers in the interval , with compensating contributions to R. Our data are in excellent agreement with recent high-field data on YBCO and LSCO. The quantitative consistency across three different cuprates shows that a drop in carrier density from to is a universal signature of the pseudogap transition at . We discuss the implication of these findings for the nature of the pseudogap phase.
arXiv comment11 pages, 12 figures
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