Field theory of spin-singlet quantum Hall states
arXiv:cond-mat/0008228 · doi:10.1103/PhysRevLett.86.882
Abstract
We formulate a field theory for a class of spin-singlet quantum Hall states (the Haldane-Rezayi state and its variants) which have been proposed for the quantized Hall plateaus observed at the second lowest Landau level. A new essential ingredient is a class of super Chern-Simons field. We show that the known properties of the states are consistently described by it. We also give a 2+1 dimensional hierarchical construction. Implications of the proposal are discussed and a new physical picture of composite particles at the second lowest Landau level emerges.
RevTex, 5 pages, 1 figure
References in corpus (10)
- Paired states of fermions in two dimensions with breaking of parity and time-reversal symmetries, and the fractional quantum Hall effect
- Transition from quantum Hall to compressible states in the second Landau level: new light on the =5/2 enigma
- Incompressible paired Hall state, stripe order and the composite fermion liquid phase in half-filled Landau levels
- Exact Quantization of Even-Denominator Fractional Quantum Hall State at =5/2 Landau Level Filling Factor
- A Chern-Simons Effective Field Theory for the Pfaffian Quantum Hall State
- Landau-Ginzburg Theories for Non-Abelian Quantum Hall States
- Singular Pair Breaking in the Composite Fermi Liquid Description of the Half-Filled Landau Level
- The Haldane-Rezayi Quantum Hall State and Magnetic Flux
- Spin-singlet hierarchy in the fractional quantum Hall effect
- Wave Function of the Largest Skyrmion on a Sphere
Cited by in corpus (5)
- Operator Product Expansion in Logarithmic Conformal Field Theory
- Non-Relativistic Supergeometry in the Moore-Read Fractional Quantum Hall State
- The O(n) Model in the Limit (self-avoiding-walks) and Logarithmic Conformal Field Theory
- Gauging or extending bulk and boundary conformal field theories: Application to bulk and domain wall problem in topological matter and their descriptions by (mock) modular covariant
- Fermionic fractional quantum Hall states: A modern approach to systems with bulk-edge correspondence