Hopf term induced by fermions
arXiv:hep-th/0005150 · doi:10.1016/S0370-2693(00)01118-7
Abstract
We derive an effective action for Dirac fermions coupled to O(3) non-linear sigma-model (NLSM) through the Yukawa-type interaction. The nonperturbative (global) quantum anomaly of this model results in a Hopf term for the effective NLSM. We obtain this term using the ``embedding'' of the CP model into the CP generalization of the model which makes the quantum anomaly perturbative. This perturbative anomaly is calculated by means of a gradient expansion of a fermionic determinant and is given by the Chern-Simons term for an auxiliary gauge field.
5 pages, no figures, latex, elsart.cls, minor errors are corrected
References in corpus (1)
Cited by in corpus (16)
- Topological delocalization of two-dimensional massless Dirac fermions
- Chiral non-linear sigma-models as models for topological superconductivity
- Soliton solutions of the fermion-Skyrmion system in (2+1) dimensions
- Fermionic Hopf solitons and Berry's phase in topological surface superconductors
- Topological terms of (2+1)d flag-manifold sigma models
- Non-abelian bosonization in two and three spatial dimensions and applications
- Generalized symmetries in singularity-free nonlinear models and their disordered phases
- Finite Temperature Induced Fermion Number In The Nonlinear sigma Model In (2+1) Dimensions
- Statistical nature of Skyrme-Faddeev models in dimensions and normalizable fermions
- Realization of the topological Hopf term in two-dimensional lattice models
- Theory of topological defects and textures in two-dimensional quantum orders with spontaneous symmetry breaking
- Collective coordinate quantization and spin statistics of the solitons in the Skyrme-Faddeev model
- A baby--Skyrme model with anisotropic DM interaction: Compact skyrmions revisited
- Topological calculation of the phase of the determinant of a non self-adjoint elliptic operator
- Fermionic skyrmions and bosonization for a Gross-Neveu transition
- Hopf symmetry protected topological phases in the vicinity of spin orders