Coherent quasi-particles-to-incoherent hole-carriers crossover in underdoped cuprates
arXiv:0806.0101 · doi:10.1103/PhysRevB.79.140502
Abstract
In underdoped cuprates, only a portion of the Fermi surface survives as Fermi arcs due to pseudogap opening. In hole-doped LaCuO, we have deduced the "coherence temperature" of quasi-particles on the Fermi arc above which the broadened leading edge position in angle-integrated photoemission spectra is shifted away from the Fermi level and the quasi-particle concept starts to lose its meaning. is found to rapidly increase with hole doping, an opposite behavior to the pseudogap temperature . The superconducting dome is thus located below both and , indicating that the superconductivity emerges out of the coherent Fermionic quasi-particles on the Fermi arc. remains small in the underdoped region, indicating that incoherent charge carriers originating from the Fermi arc are responsible for the apparently metallic transport at high temperatures.
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- A Phenomenological Theory of the Anomalous Pseudogap Phase in Underdoped Cuprates
- A Tale of Two Metals: contrasting criticalities in the pnictides and hole-doped cuprates
- Quasiparticles in the Pseudogap Phase of Underdoped Cuprate
- Andreev and Single Particle Tunneling Spectroscopies in Underdoped Cuprates
- Commensurate and incommensurate magnetic order in the doped two-dimensional Hubbard model: dynamical mean-field theory analysis
- Strange metal from incoherent bosons
- On the Origin of the Checkerboard Pattern in Scanning Tunneling Microscopy Maps of Underdoped Cuprate Superconductors
- Temperature evolution of correlation strength in the superconducting state of high-Tc cuprates
- Enhanced Josephson tunneling between high temperature superconductors through a normal pseudogap underdoped cuprate with a finite energy cooperon
- Yamaji effect and quantum oscillation in Yang-Rice-Zhang model of underdoped cuprates
- Superconductivity driven by pairing of the coherent parts of the physical electrons