Spin Liquid States at the vicinity of metal-insulator transition
arXiv:1302.0157 · doi:10.1103/PhysRevB.88.165130
Abstract
We study in this paper quantum spin liquid states (QSLs) at the vicinity of metal-insulator transition. Assuming that the low energy excitations in the QSLs are labeled by "spinon" occupation numbers with the same Fermi surface structure as in the corresponding metal (Fermi-liquid) side, we propose a phenomenological Landau-like low energy theory for the QSLs and show that the usual U(1) QSLs is a representative member of this class of spin liquids. Based on our effective low energy theory, an alternative picture to the Brinkman-Rice picture of Mott metal-insulator transition is proposed. The charge, spin and thermal responses of QSLs are discussed under such a phenomenology.
8 pages, extended version to appear in PRB
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- U(1) Gauge Theory of the Hubbard Model : Spin Liquid States and Possible Application to k-(BEDT-TTF)_2 Cu_2 (CN)_3
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- Transport Properties of a spinon Fermi surface coupled to a U(1) gauge field
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- Absence of magnetic thermal conductivity in the quantum spin liquid candidate EtMe3Sb[Pd(dmit)2]2 -- revisited
- Quasi-continuous transition from a Fermi liquid to a spin liquid
- Field-Induced Instability of a Gapless Spin Liquid with a Spinon Fermi Surface
- Electrodynamics of quantum spin liquids
- Cyclotron resonance inside the Mott gap: a fingerprint of emergent neutral fermions
- Low-Energy Excitations in Quantum Spin-Liquids Identified by Optical Spectroscopy
- Distinct-symmetry spin liquid states and phase diagram of Kitaev-Hubbard model
- Persistence of fermionic spin excitations through a genuine Mott transition in -type organics
- Optical conductivity and surface plasmon modes of U(1) spin liquid states with large spinon Fermi surfaces
- Fractionalization of long-range ordered states in a Falicov-Kimball model
- Continuous transition from a Landau quasiparticle to a neutral spinon
- Nonlinear optical conductivity of spin liquids with large spinon Fermi surfaces
- Collective effects in an incompressible electronic liquid