Laughlin states and their quasi-particle excitations on the torus
arXiv:1405.0742 · doi:10.1103/PhysRevB.93.245156
Abstract
We provide a full derivation of Laughlin's Jastrow-type wave functions for quantized Hall states subject to periodic boundary conditions using an operator formalism. The construction includes the quasi-hole and the technically more challenging quasi-electron excitation, which was left as an open problem in the classic paper by Haldane and Rezayi [Phys. Rev. B 31, 2529 (1985)].
11 pages, no figures
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- Origin of the fractional quantum Hall effect in wide quantum wells
- Quasielectrons in lattice Moore-Read models
- On the modular covariance properties of composite fermions on the torus
- Continuum limit of lattice quasielectron wavefunctions
- Anisotropy and quench dynamics of quasiholes in fractional quantum Hall liquids