The pseudogap ground state in high temperature superconductors
arXiv:0803.1884 · doi:10.1103/PhysRevB.78.140506
Abstract
By re-examining recently-published data from angle-resolved photoemission spectroscopy we demonstrate that, in the superconducting region of the phase diagram, the pseudogap ground state is an arc metal. This scenario is consistent with results from Raman spectroscopy, specific heat and NMR. In addition, we propose an explanation for the "Fermi pockets" inferred from quantum oscillations in terms of a pseudogapped bilayer Fermi surface.
4 pages, 3 figures, added discussion of NMR and optical conductivity data, submitted to Physical Review B as a rapid communication
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Cited by in corpus (15)
- Thermodynamic signatures of quantum criticality in cuprates
- The electronic specific heat of Ba1-xKxFe2As2 (x=0 to 1.0) from 2K to 380K
- Dielectric versus magnetic pairing mechanisms in high-temperature cuprate superconductors investigated using Raman scattering
- Specific heat of underdoped cuprates: RVB versus Fermi arcs
- Coexistence of the superconducting energy gap and pseudogap above and below the transition temperature of superconducting cuprates
- Locating the pseudogap closing point in cuprate superconductors: absence of entrant or reentrant behavior
- Lifshitz quantum phase transitions and Fermi surface transformation with hole doping in high- superconductors
- Electron pockets and pseudogap asymmetry observed in the thermopower of underdoped cuprates
- Kinetics of excitations on the Fermi arcs in underdoped cuprates at low temperature
- Doping and temperature dependence of the pseudogap and Fermi arcs in cuprates from -CDW short-range fluctuations in the context of the t-J model
- Energy gaps in high- superconductors: BCS after all?
- Tc is insensitive to magnetic interactions in high-Tc superconductors
- Fermi arcs and isotope effect of the magnetic penetration depth in underdoped cuprates
- The pseudogap in hole-doped cuprates: possible insights from the Kondo effect
- Stranger than Metals