Bosonization with a background gauge field
arXiv:1902.06584 · doi:10.1103/PhysRevB.100.075105
Abstract
Bosonization is one of the most significant frameworks to analyze fermionic systems. In this work, we propose a new bosonization of Dirac fermion coupled with background gauge field consistent with gauge invariance, global chiral anomaly matching and fermion-boson operator correspondence, either of which is not satisfied by previously developed bosonizations. The bilinear Dirac-mass term condensation paradox and its generalized form are resolved by our bosonization. This new bosonization approach to interacting systems also correctly captures the conformal characters of a significant class of critical lattice models, such as conformal dimensions and conformal anomaly of XXZ spin chain with twisted boundary condition. Our work clarifies the equivalence of fermionic flux insertion and bosonic background charge insertion for two-dimensional conformal field theory.
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References in corpus (7)
- Non-Abelian Anyons and Topological Quantum Computation
- Generalized Global Symmetries
- Symmetric-Gapped Surface States of Fractional Topological Insulators
- Lieb-Schultz-Mattis type theorem with higher-form symmetry and the quantum dimer models
- Insensitivity of bulk properties to the twisted boundary condition
- Scaling of polarization amplitude in quantum many-body systems in one dimension
- Polarization amplitude near quantum critical points
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- Kubo's response theory and bosonization with a background gauge field and irrelevant perturbations
- Lieb-Schultz-Mattis constraints for the insulating phases of the one-dimensional SU() Kondo lattice model