A consistent field theoretical formulation of fermionic matter coupled to a non-abelian Chern Simons terms is usually regarded as problematic due to the violation of (classical) Poincare covariance. We discuss an alternative Hamiltonian formalism, developed by Faddeev Jackiw and Dirac, which overcom
The Braid Group of a Canonical Chern-Simons Theory on a Riemann Surface
β Scribed by Mario Bergeron; Gordon Semenoff
- Publisher
- Elsevier Science
- Year
- 1996
- Tongue
- English
- Weight
- 689 KB
- Volume
- 245
- Category
- Article
- ISSN
- 0003-4916
No coin nor oath required. For personal study only.
β¦ Synopsis
We examine the problem of determining which representations of the braid group on a Riemann surface and carried by the wave function of a quantized Abelian Chern Simons theory interacting with spinless non-dynamical matter. We generalize the quantization of Chern Simons theory to the case where the coefficient of the Chern Simons term, k, is rational (for a set of rational charges), the Riemann surface has arbitrary genus, and the total matter charge is non-vanishing. We find an explicit solution of the Schro dinger equation. We find that the wave functions carry a representation of the braid group as well as a dual projective representation of the discrete group of large gauge transformations. We find a fundamental constraint which relates the charges of the particles, q i , the coefficient k and the genus of the manifold, g : q i (Q+q i ( g&1))Γk is integer (where Q is the total charge).
π SIMILAR VOLUMES
Let X , be a geometrically connected smooth and proper curve over a local or global field K . Following GROTHENDIECK [3] there is a canonical exact sequence for the (etale) fundamental group z,(X,) of X,. (Here and in the following we will omit the base points.) where I? denotes an algebraic closur
Let + be an orthogonal measure with compact support of finite length in C n . We prove, under a very weak hypothesis of regularity on the support (Supp +) of +, that this measure is characterized by its boundary values (in the weak sense of currents) of the current [T] 7 ., where T is an analytic su