Confinement transition to density wave order in metallic doped spin liquids
arXiv:1602.05954 · doi:10.1103/PhysRevB.93.165139
Abstract
Insulating quantum spin liquids can undergo a confinement transition to a valence bond solid state via the condensation of topological excitations of the associated gauge theory. We extend the theory of such transitions to fractionalized Fermi liquids (FL*): these are metallic doped spin liquids in which the Fermi surfaces only have gauge neutral quasiparticles. Using insights from a duality transform on a doped quantum dimer model for the U(1)-FL* state, we show that projective symmetry group of the theory of the topological excitations remains unmodified, but the Fermi surfaces can lead to additional frustrating interactions. We propose a theory for the confinement transition of -FL* states via the condensation of visons. A variety of confining, incommensurate density wave states are possible, including some that are similar to the incommensurate -form factor density wave order observed in several recent experiments on the cuprate superconductors.
31 pages, 8 figures, to appear in Phys. Rev. B
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- Probing the pseudogap and beyond: Examining single-particle properties of the hole- and electron-doped Hubbard model
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