Systematic Low-Energy Effective Field Theory for Magnons and Holes in an Antiferromagnet on the Honeycomb Lattice
arXiv:1109.1419 · doi:10.1103/PhysRevB.85.075123
Abstract
Based on a symmetry analysis of the microscopic Hubbard and t-J models, a systematic low-energy effective field theory is constructed for hole-doped antiferromagnets on the honeycomb lattice. In the antiferromagnetic phase, doped holes are massive due to the spontaneous breakdown of the symmetry, just as nucleons in QCD pick up their mass from spontaneous chiral symmetry breaking. In the broken phase the effective action contains a single-derivative term, similar to the Shraiman-Siggia term in the square lattice case. Interestingly, an accidental continuous spatial rotation symmetry arises at leading order. As an application of the effective field theory we consider one-magnon exchange between two holes and the formation of two-hole bound states. As an unambiguous prediction of the effective theory, the wave function for the ground state of two holes bound by magnon exchange exhibits -wave symmetry.
33 pages, 6 figures
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Cited by in corpus (8)
- Low-Temperature Properties of Two-Dimensional Ideal Ferromagnets
- Thermodynamics of Two-Dimensional Ideal Ferromagnets - Three-Loop Analysis
- Symmetry Analysis of Holes Localized on a Skyrmion in a Doped Antiferromagnet
- Low-Temperature Properties of Ferromagnetic Spin Chains in a Magnetic Field
- Thermodynamics of Ferromagnetic Spin Chains in a Magnetic Field: Impact of the Spin-Wave Interaction
- Systematic Effective Field Theory Analysis of the D=2+1 Quantum XY Model at Low Temperatures
- Holes Localized on a Skyrmion in a Doped Antiferromagnet on the Honeycomb Lattice: Symmetry Analysis
- Thermodynamics of the =3+1 Quantum XY Model