2005/04/30 by Arkadiusz Wojs, Arkadiusz Wójs, Daniel Wodzinski +2 · 2 citations
Mathematics · Physics and Astronomy · #Cluster (spacecraft) #Cluster size #Combinatorics #Composite fermion #Composite number #Computer science #Condensed matter physics #Distribution (mathematics) #Electron #Electronic structure #Fermion #Fractional quantum Hall effect #Landau quantization #Magnetic properties of thin films #Mathematical analysis #Mathematical physics #Mathematics #Physics #Physics of Superconductivity and Magnetism #Quantum Hall effect #Quantum and electron transport phenomena #Quantum mechanics #Quantum spin Hall effect #cond-mat.mes-hall
paper · pdf · doi:10.1103/physrevb.71.245331
published as Phys.Rev. B71 (2005) 245331 · submitted to PRB
arxiv created 2005/04/30 · openalex publication_date 2005/06/30 · arxiv updated 2009/12/01 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/05
Pair-distribution functions g(r) of Laughlin quasielectrons (composite fermions in their second Landau level) are calculated in the fractional quantum Hall states at electron filling factors \ensuremathνe=4∕11 and 3∕8. A shoulder in g(r) is found, supporting the idea of cluster formation. The intra- and intercluster contributions to g(r) are identified, largely independent of \ensuremathνe. The average cluster sizes are estimated; pairs and triplets of quasielectrons are suggested at \ensuremathνe=4∕11 and 3∕8, respectively.