English

Generalized CP^1 model from t_1-t_2-J model

Condensed Matter 2016-08-31 v1

Abstract

A long-wavelength, low-frequency effective theory is obtained from t1t2Jt_1-t_2-J model. The action is written in terms of two-component bose spinor fields (CP^1 fields) and two spinless Fermi fields. The generalized CP^1 model is invariant under U(1) gauge transformations. The bose fields and one of the Fermi fields have charge +1 while the other Fermi field has charge -1 with respect to these transformations. A simple mean-feild theory of a gauge-symmerty breaking, based on a four-fermion interaction, is discussed. An effective theory of frustrated antiferromagnetism is obtained integrating out the Fermi fields around the mean-fields. Another option is used to parametrize the long distance fluctuations in t1t2Jt_1-t_2-J model, with the help of gauge invariant fields. It is argued that the resulting Fermi quasiparticles of the t1t2Jt_1-t_2-J model have both charge and spin. The effective action is rewritten in terms of spin 1/2 Fermi spinor, which has the charge of the holes, and unit vector.

Keywords

Cite

@article{arxiv.cond-mat/9706105,
  title  = {Generalized CP^1 model from t_1-t_2-J model},
  author = {Naoum Karchev},
  journal= {arXiv preprint arXiv:cond-mat/9706105},
  year   = {2016}
}

Comments

22 pages, RevTex, no figures

R2 v1 2026-07-22T11:58:07.366Z