Linear differential equations for a fractional spin field

Nov, 1992
14 pages
Published in:
  • J.Math.Phys. 35 (1994) 6049-6057
e-Print:
Report number:
  • DFTUZ-92-24-REV,
  • DFTUZ-92-24

Citations per year

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Abstract:
The vector system of linear differential equations for a field with arbitrary fractional spin is proposed using infinite-dimensional half-bounded unitary representations of the SL(2,R)\overline{SL(2,R)} group. In the case of (2j+1)(2j+1)-dimensional nonunitary representations of that group, 0<2jZ0<2j\in Z, they are transformed into equations for spin-jj fields. A local gauge symmetry associated to the vector system of equations is identified and the simplest gauge invariant field action, leading to these equations, is constructed.
Note:
  • Revised version
  • anyon
  • spin: fractional
  • field equations: solution
  • group theory: representation
  • symmetry: SL(2,R)
  • gauge field theory: action
  • dimension: 3