Bilayer mapping of the paired quantum Hall state: Instability toward anisotropic pairing
arXiv:1412.2430 · doi:10.1103/PhysRevB.91.195119
Abstract
One of the most dominant candidates for the paired quantum Hall (QH) state at filling factor is the Moore-Read (MR) Pfaffian state. A salient problem, however, is that it does not occur exactly at the Coulomb interaction, but rather at a modified interaction, which favors particle-hole symmetry breaking. In an effort to find a better state, in this work, we investigate the possible connection between the paired QH state and the antisymmetrized bilayer ground state, which is inspired by the intriguing identity that the MR Pfaffian state is entirely equivalent to the antisymmetrized projection of the bilayer QH state called the Halperin (331) state, which is valid at interlayer distance, , roughly equal to the magnetic length, . Specifically, by using exact diagonalization in the torus geometry, we show that the exact state at a given Haldane pseudopotential variation is intimately connected with the antisymmetrized bilayer ground state at a corresponding via one-to-one mapping, which we call the bilayer mapping. One of the most important discoveries in this work is that the paired QH state occurring at the Coulomb interaction is mapped onto the antisymmetrized bilayer ground state at , which is equivalent to the antisymmetrized product state of two composite fermion seas at quarter filling, not the MR Pfaffian state. While maintaining high overlap with the paired QH state, the antisymmetrized bilayer ground state at exhibits an abrupt change under the influence of small anisotropy. This suggests that the paired QH state occurring at the Coulomb interaction might be susceptible to anisotropic instability, opening up the possibility of anisotropic or -wave pairing instead of -wave pairing in the MR Pfaffian/anti-Pfaffian state.
18 pages, 8 figures
References in corpus (20)
- Non-Abelian Anyons and Topological Quantum Computation
- Particle-hole symmetry and the Pfaffian state
- Particle-Hole Symmetry and the Quantum Hall State
- Infinite density matrix renormalization group for multicomponent quantum Hall systems
- Finite Layer Thickness Stabilizes the Pfaffian State for the 5/2 Fractional Quantum Hall Effect: Wavefunction Overlap and Topological Degeneracy
- Density Matrix Renormalization Group Study of Incompressible Fractional Quantum Hall States
- Half-Filled Lowest Landau Level on a Thin Torus
- Band mass anisotropy and the intrinsic metric of fractional quantum Hall systems
- Intrinsic Gap of the nu=5/2 Fractional Quantum Hall State
- Gauge-Fixed Wannier Wave-Functions for Fractional Topological Insulators
- Paired composite fermion wavefunctions
- The Phase Diagram of the Fractional Quantum Hall Effect: Effects of Landau Level Mixing and Non-Zero Width
- Orbital Landau level dependence of the fractional quantum Hall effect in quasi-two dimensional electron layers: finite-thickness effects
- Fractional Quantum Hall Effect at Landau Level Filling nu=4/11
- Fractional quantum Hall states in two-dimensional electron systems with anisotropic interactions
- Spontaneous Particle-Hole Symmetry Breaking in the Fractional Quantum Hall Effect
- Halperin (m, m',n) bilayer quantum Hall states on thin cylinders
- Quantum Phase Transitions and the ν=5/2 Fractional Hall State in Wide Quantum Wells
- Fractional quantum Hall effects in bilayers in the presence of inter-layer tunneling and charge imbalance
- Superconducting Order Parameter for the Even-denominator Fractional Quantum Hall Effect
Cited by in corpus (4)
- Fractional Quantum Hall Bilayers at Half-Filling: Tunneling-driven Non-Abelian Phase
- Onset of Quantum Criticality in the Topological-to-Nematic Transition in a Two-dimensional Electron Gas at Filling Factor
- Nematic fluctuations balancing the zoo of phases in half-filled quantum Hall systems
- Exploring Quantum Hall Physics at Ultra-Low Temperatures and at High Pressures