Two Pseudogaps in the Cuprates: Meingast et al. Reply
arXiv:cond-mat/0307203 · doi:10.1103/PhysRevLett.89.229704
Abstract
In classical superconductors Cooper-pair formation and phase coherence occur simultaneously as the temperature is lowered below Tc. In high-temperature superconductors (HTSC), on the other hand, the small superfluid density and low associated phase stiffness of the superconducting condensate are expected to lead to a separation of the Cooper-pair formation and the phase-coherence temperatures, especially in underdoped materials [3]. The only real phase transition in this scenario is the 3d-XY phase-ordering transition at Tc [3,4]. In our Letter [2] we showed that Tc in underdoped and optimally doped YBCO is just such a phase-ordering temperature, and then the question naturally arises - where do the Cooper pairs form? The observed 3d-XY scaling of our thermal expansion data over a wide temperature range [2] suggests that pairing occurs at temperatures considerably above Tc, and it thus appeared quite natural for us to associate the opening of the pseudogap at T*.
3 pages, 1 Figure (Reply to Comment by R. S. Markiewicz, Phys. Rev. Lett. 89, 229703 (2002)
References in corpus (6)
- The onset of the vortex-like Nernst signal above Tc in La_{2-x}Sr_xCuO_4 and Bi_2Sr_{2-y}La_yCuO_6
- Extreme Type-II Superconductors in a Magnetic Field: A Theory of Critical Fluctuations
- Chiral Symmetry Breaking and Phase Fluctuations in Cuprate Superconductors: A QED Unified Theory of the Pseudogap State
- Phase fluctuations and the pseudogap in YBa2Cu3Ox
- Magnetic Field Effect on the Pseudogap Temperature within Precursor Superconductivity
- Two Pseudogaps in the Cuprates
Cited by in corpus (4)
- Developments in the negative-U modelling of the cuprate HTSC systems
- Evolution of the specific-heat anomaly of the high-temperature superconductor YBa2Cu3O7 under influence of doping through application of pressure up to 10 GPa
- Magnetic field induced enlargement of the regime of critical fluctuations in the classical superconductor V3Si from high-resolution specific heat experiments
- Magnetic field induced 3D to 1D crossover in type II superconductors