Umklapp scattering as the origin of -linear resistivity in the normal state of high- cuprate superconductors
arXiv:1707.05666 · doi:10.1103/PhysRevB.96.220502
Abstract
The high-temperature normal state of the unconventional cuprate superconductors has resistivity linear in temperature , which persists to values well beyond the Mott-Ioffe-Regel upper bound. At low-temperature, within the pseudogap phase, the resistivity is instead quadratic in , as would be expected from Fermi liquid theory. Developing an understanding of these normal phases of the cuprates is crucial to explain the unconventional superconductivity. We present a simple explanation for this behavior, in terms of umklapp scattering of electrons. This fits within the general picture emerging from functional renormalization group calculations that spurred the Yang-Rice-Zhang ansatz: umklapp scattering is at the heart of the behavior in the normal phase.
v1 6+1 pages, 4 figures; v2 6+2 pages, 4 figures; v3 6 + 2.5 pages, 5 figures
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- Low-temperature T resistivity in the underdoped pseudogap phase versus T-linear resistivity in the overdoped strange-metal phase of cuprate superconductors
- Two -linear scattering rate regimes in the triangular lattice Hubbard model
- Interaction-enhanced nesting in Spin-Fermion and Fermi-Hubbard models
- Thermoelectric power of overdoped Tl2201 crystals: Charge density waves and and resistivities
- Correlation between the strength of low-temperature T-linear normal-state resistivity and in overdoped electron-doped cuprate superconductors
- Yamaji effect and quantum oscillation in Yang-Rice-Zhang model of underdoped cuprates
- Minimal one-dimensional model of bad metal behavior from fast particle-hole scattering
- Impurity-Scattering Assisted Umklapp Scattering as the Origin of Low-Temperature Resistivity in the Normal-State of Cuprate Superconductors