Fractionalized Fermi liquid with bosonic chargons as a candidate for the pseudogap metal
arXiv:1607.05727 · doi:10.1103/PhysRevB.94.205117
Abstract
Doping a Mott-insulating spin liquid can lead to a fractionalized Fermi liquid (FL*). Such a phase has several favorable features that make it a candidate for the pseudogap metal for the underdoped cuprates. We focus on a particular, simple -FL* state which can undergo a confinement transition to a spatially uniform superconductor which is smoothly connected to the `plain vanilla' BCS superconductor with -wave pairing. Such a transition occurs by the condensation of bosonic particles carrying charge but no spin (`chargons'). We show that modifying the dispersion of the bosonic chargons can lead to confinement transitions with charge density waves and pair density waves at the same wave-vector , co-existing with -wave superconductivity. We also compute the evolution of the Hall number in the normal state during the transition from the plain vanilla FL* state to a Fermi liquid, and argue, following Coleman, Marston, and Schofield [Phys. Rev. B 72, 245111 (2005)], that it exhibits a discontinuous jump near optimal doping. We note the distinction between these results and those obtained from models of the pseudogap with fermionic chargons.
25 + 5 pages, 7 figures, 1 table; (v2) 25 + 6 pages, 7 figures, 1 table, added clarifications and discussion on stability of phases
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- Hall effect in cuprates with incommensurate spin-density wave
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- Emergence of nodal Bogoliubov quasiparticles across the transition from the pseudogap metal to the d-wave superconductor
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- Yamaji effect in models of underdoped cuprates
- Yamaji effect and quantum oscillation in Yang-Rice-Zhang model of underdoped cuprates
- Probing the pseudogap and beyond: Examining single-particle properties of the hole- and electron-doped Hubbard model
- Exploring Strongly Interacting Gapless States: Cuprates, Pair Density Waves, and Fluctuating Superconductivity
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