Non-local matrix generalizations ofW-algebras |
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Authors: | Adel Bilal |
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Institution: | (1) Joseph Henry Laboratories, Princeton University, 08544 Princeton, NJ, USA;(2) Present address: Laboratoire de Physique Théorique de l'Ecole Normale Supériure, 24 rue Lhomond, 75231 Paris Cedex 05, France |
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Abstract: | There is a standard way to define two symplectic (hamiltonian) structures, the first and second Gelfand-Dikii brackets, on the space of ordinarym
th-order linear differential opeatorsL=–d
m
+U
1
d
m–1+U
2
d
m–2+...+U
m
. In this paper, I consider in detail the case where theU
k
aren×n-matrix-valued functions, with particular emphasis on the (more interesting) second Gelfand-Dikii bracket. Of particular interest is the reduction to the symplectic submanifoldU
1=0. This reduction gives rise to matrix generalizations of (the classical version of) thenon-linear W
m
-algebras, calledV
n, m
-algebras. The non-commutativity of the matrices leads tonon-local terms in theseV
n, m
-algebra.s I show that these algebras contain a conformal Virasoro subalgebra and that combinationsW
k
of theU
k
can be formed that aren×n-matrices of conformally primary fields of spink, in analogy with the scalar casen=1. In general however, theV
m, n
-algebras have a much richer structure than theW
m
-algebras as can be seen on the examples of thenon-linear andnon-local Poisson brackets {(U
2)ab(), (U
2)cd()}, {(U
2)ab(), (W
3)cd()} and {(W
3)ab(), (W
3)cd()} which I work out explicitly for allm andn. A matrix Miura transformations is derived, mapping these complicated (second Gelfand-Dikii) brackets of theU
k
to a set of much simpler Poisson brackets, providing the analogoue of the free-field representation of theW
m
-algebras. |
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Keywords: | |
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