Non-1/m fractional quantum Hall effect is a manifestation of anyon superconductivity
- Texas A and M Univ., College Station, TX (United States). Dept. of Physics
This paper reports that regarding electrons as anyons of index {alpha}{sub s} with {minus}(m + {alpha}{sub s}) flux quanta per particle, and letting the mean field of these fluxes cancel the external magnetic field B, the authors obtain the filling factor {nu} = 1/(m + {alpha}{sub s}), where m must be odd. Demanding the resulting system of anyons to exhibit anyon superconductivity, we obtain {alpha}{sub s} = {plus minus}(1 {minus} q/n) where q is odd, and n {gt} q is relatively prime to q. For q = 1 the authors recover a formula due to Jain, and resolve the mystery why, for a state with {nu} = n/(2pn {plus minus} 1) {lt} 1 he requires use of the statistical correlation of n filled Landau levels. For q = 3,5,..., we obtain the fractions 4/11, 4/13, 5/13, etc., which are missing from Jain's list. Thus this non-hierarchical approach to the non-1/m fractional quantum Hall effect has the strengths of Jain's composite-fermion approach, but not its (potential) weaknesses.
- OSTI ID:
- 5295549
- Journal Information:
- International Journal of Modern Physics B; (United States), Vol. 5:10; ISSN 0217-9792
- Country of Publication:
- United States
- Language:
- English
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Related Subjects
SUPERCONDUCTIVITY AND SUPERFLUIDITY
SUPERCONDUCTIVITY
ANYONS
COMPOSITE MODELS
CORRELATION FUNCTIONS
ELECTRONS
EQUATIONS
FERMIONS
HALL EFFECT
MAGNETIC FLUX
POTENTIALS
QUANTUM MECHANICS
STATISTICAL MECHANICS
ELECTRIC CONDUCTIVITY
ELECTRICAL PROPERTIES
ELEMENTARY PARTICLES
FUNCTIONS
LEPTONS
MATHEMATICAL MODELS
MECHANICS
PARTICLE MODELS
PHYSICAL PROPERTIES
QUASI PARTICLES
665411* - Basic Superconductivity Studies- (1992-)