1997/11/11 by Eduardo Fradkin, E. Fradkin, Chetan Nayak +3 · 12 citations
Mathematics · Physics and Astronomy · #Chern–Simons theory #Coupling constant #Effective field theory #Electron #Fractional quantum Hall effect #Gauge theory #Mathematical physics #Mathematics #Pfaffian #Physics #Physics of Superconductivity and Magnetism #Pure mathematics #Quantum Hall effect #Quantum and electron transport phenomena #Quantum field theory #Quantum mechanics #Quantum spin Hall effect #Quasiparticle #Theoretical physics #Topological Materials and Phenomena #cond-mat.mes-hall
paper · pdf · doi:10.1016/s0550-3213(98)00111-4
published as Nucl.Phys. B516 (1998) 704-718 · 10 pages, LaTeX, 3 eps figures
arxiv created 1997/11/11 · openalex publication_date 1998/04/01 · arxiv updated 2009/11/30 · openalex created_date 2016/06/24 · openalex updated_date 2026/08/05
We present a low-energy effective field theory describing the universality class of the Pfaffian quantum Hall state. To arrive at this theory, we observe that the edge theory of the Pfaffian state of bosons at ν=1 is an SU(2)2 Kac-Moody algebra. It follows that the corresponding bulk effective field theory is an SU(2) Chern-Simons theory with coupling constant k=2. The effective field theories for other Pfaffian states, such as the fermionic one at ν=1/2 are obtained by a flux-attachment procedure. We discuss the non-Abelian statistics of quasiparticles in the context of this effective field theory.