A dipole interpretation of the \(\nu=1/2\) state

DOI10.1016/S0550-3213(98)00069-8zbMath0947.81572arXivcond-mat/9712169OpenAlexW2600355846MaRDI QIDQ1382379

Vincent Pasquier, F. Duncan M. Haldane

Publication date: 25 March 1998

Published in: Nuclear Physics. B (Search for Journal in Brave)

Full work available at URL: https://arxiv.org/abs/cond-mat/9712169

zbMATH Keywords

lowest Landau levelmean field approximationstrong magnetic fieldbosonic particlesinteracting fermion

Mathematics Subject Classification ID

Many-body theory; quantum Hall effect (81V70)

Related Items (9)

Jain states in a matrix theory of the quantum Hall effect ⋮ A note on broken dilatation symmetry in planar noncommutative theory ⋮ EXPLANATION OF COMPOSITE FERMION STRUCTURE IN FRACTIONAL QUANTUM HALL SYSTEMS ⋮ Composite fermion metals from dyon black holes and S-duality ⋮ Hamiltonian theories of the fractional quantum Hall effect ⋮ W-infinity symmetry in the quantum Hall effect beyond the edge ⋮ The last word in strong correlations ⋮ ‘One-dimensional’ theory of the quantum Hall system ⋮ Effective Hamiltonian for striped and paired states at the half-filled Landau level

This page was built for publication: A dipole interpretation of the \(\nu=1/2\) state