English

Non-Local Matrix Generalizations of W-Algebras

High Energy Physics - Theory 2009-10-28 v2 funct-an Functional Analysis

Abstract

There is a standard way to define two symplectic (hamiltonian) structures, the first and second Gelfand-Dikii brackets, on the space of ordinary linear differential operators of order mm, L=dm+U1dm1+U2dm2++UmL = -d^m + U_1 d^{m-1} + U_2 d^{m-2} + \ldots + U_m. In this paper, I consider in detail the case where the UkU_k are n×nn\times n-matrix-valued functions, with particular emphasis on the (more interesting) second Gelfand-Dikii bracket. Of particular interest is the reduction to the symplectic submanifold U1=0U_1=0. This reduction gives rise to matrix generalizations of (the classical version of) the {\it non-linear} WmW_m-algebras, called Vm,nV_{m,n}-algebras. The non-commutativity of the matrices leads to {\it non-local} terms in these Vm,nV_{m,n}-algebras. I show that these algebras contain a conformal Virasoro subalgebra and that combinations WkW_k of the UkU_k can be formed that are n×nn\times n-matrices of conformally primary fields of spin kk, in analogy with the scalar case n=1n=1. In general however, the Vm,nV_{m,n}-algebras have a much richer structure than the WmW_m-algebras as can be seen on the examples of the {\it non-linear} and {\it non-local} Poisson brackets of any two matrix elements of U2U_2 or W3W_3 which I work out explicitly for all mm and nn. A matrix Miura transformation is derived, mapping these complicated second Gelfand-Dikii brackets of the UkU_k to a set of much simpler Poisson brackets, providing the analogue of the free-field realization of the WmW_m-algebras.

Keywords

Cite

@article{arxiv.hep-th/9403197,
  title  = {Non-Local Matrix Generalizations of W-Algebras},
  author = {Adel Bilal},
  journal= {arXiv preprint arXiv:hep-th/9403197},
  year   = {2009}
}

Comments

43 pages, a reference and a remark on the conformal properties for $U_1\ne 0$ added