Abstract

In the cuprate superconductors, Nernst and torque magnetization experiments have provided evidence that the disappearance of the Meissner effect at TcT_c is caused by the loss of long-range phase coherence, rather than the vanishing of the pair condensate. Here we report a series of torque magnetization measurements on single crystals of La2−xSrxCuO4\mathrm{La_{2-x}Sr_xCuO_4} (LSCO), Bi2Sr2−yLayCuO6\mathrm{Bi_2Sr_{2-y}La_yCuO_6} (Bi 2201), Bi2Sr2CaCu2O8+δ\mathrm{Bi_2Sr_2CaCu_2O_{8+δ}} (Bi 2212) and optimal YBa2Cu3O7\mathrm{YBa_2Cu_3O_7}. Some of the measurements were taken to fields as high as 45 T. Focusing on the magnetization above TcT_c, we show that the diamagnetic term MdM_d appears at an onset temperature TonsetMT^M_{onset} high above TcT_c. We construct the phase diagram of both LSCO and Bi 2201 and show that TonsetMT^M_{onset} agrees with the onset temperature of the vortex Nernst signal TonsetνT^ν_{onset}. Our results provide thermodynamic evidence against a recent proposal that the high-temperature Nernst signal in LSCO arises from a quasiparticle contribution in a charge-ordered state.

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