Conformal symmetry and universal properties of quantum Hall states

Oct, 1992
46 pages
Published in:
  • Nucl.Phys.B 398 (1993) 531-567
e-Print:
Report number:
  • CERN-TH-6702-92

Citations per year

1993200120092017202402468
Abstract:
The low-lying excitations of a quantum Hall state on a disk geometry are edge excitations. Their dynamics is governed by a conformal field theory on the cylinder defined by the disk boundary and the time variable. We give a simple and detailed derivation of this conformal field theory for integer filling, starting from the microscopic dynamics of (2+1)(2+1)-dimensional non-relativistic electrons in Landau levels. This construction can be generalized to describe Laughlin's fractional Hall states via chiral bosonization, thereby making contact with the effective Chern-Simons theory approach. The conformal field theory dictates the finite-size effects in the energy spectrum. An experimental or numerical verification of these universal effects would provide a further confirmation of Laughlin's theory of incompressible quantum fluids.
  • Hall effect
  • excited state
  • field theory: conformal
  • effect: finite size
  • thermodynamics
  • symmetry: conformal
  • boson: chiral
  • quantization
  • statistics: fractional
  • fermion: Weyl