Composite quasiparticle formation and the low-energy effective Hamiltonians of the one- and two-dimensional Hubbard Model
arXiv:cond-mat/9512090 · doi:10.1103/PhysRevB.54.7737
Abstract
We investigate the effect of hole doping on the strong-coupling Hubbard model at half-filling in spatial dimensions . We start with an antiferromagnetic mean-field description of the insulating state, and show that doping creates solitons in the antiferromagnetic background. In one dimension, the soliton is topological, spinless, and decoupled from the background antiferromagnetic fluctuations at low energies. In two dimensions and above, the soliton is non-topological, has spin quantum number 1/2, and is strongly coupled to the antiferromagnetic fluctuations. We derive the effective action governing the quasiparticle motion, study the properties of a single carrier, and comment on a possible description at finite concentration.
arXiv commentREVTEX 3.0, 22 pages with 14 figures in the PostScript format compressed using uufile. Submitted to Phys. Rev. B. The complete PostScript file including figures can be obtained via ftp at ftp://serval.berkeley.edu/hubbard.ps . It is also available via www at http://roemer.fys.ku.dk/recent.htm
References in corpus (7)
- Correlated Electrons in High Temperature Superconductors
- Quasiparticle Dispersion of the 2D Hubbard Model: From an Insulator to a Metal
- Quasiparticle dispersion of the t-J and Hubbard models
- Dynamical Properties of a Single Hole in an Antiferromagnet
- Validity of the rigid band picture for the t-J model
- Spin bags in the doped t-J model
- Quasiparticle structure and coherent propagation in the model