Abstract
A new order parameter with a novel broken symmetry is proposed for the fractional quantum Hall effect, with the Laughlin state as the mean-field ground state. The classical Ginzburg-Landau theory of Girvin is derived microscopically from this starting point and exhibits all the phenomenology of the fractional quantum Hall effect.
- Received 15 August 1988
DOI:https://doi.org/10.1103/PhysRevLett.62.86
©1989 American Physical Society