1993
DOI: 10.1142/s0217732393000738
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Deformation of the Wakimoto Construction

Abstract: We present the extension of the Wakimoto construction to the Uq( su (2)k) quantum current algebra and its associated Zk quantum parafermion algebra. This construction is achieved in terms of various deformations of three classical free boson fields. We also give the vertex operators corresponding to the quantum spin-j representation.

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Cited by 35 publications
(89 citation statements)
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References 18 publications
(32 reference statements)
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“…[9,10,11,12]. This vertex plays a role of an annihilation operator (it's anti-pode dual plays a creation operator) of physical particle in the spin k/2 XXZ model.…”
mentioning
confidence: 99%
“…[9,10,11,12]. This vertex plays a role of an annihilation operator (it's anti-pode dual plays a creation operator) of physical particle in the spin k/2 XXZ model.…”
mentioning
confidence: 99%
“…where W r is a certain submodule of F r specified as a kernel of a certain operator, called qWakimoto module [15,12,13,11,1], V (l) is the irreducible representation of U q (sl 2 ) with spin l/2 and V…”
Section: Remarkmentioning
confidence: 99%
“…One had to wait for advances in two-dimensional conformal field theory to see how the infinite two-dimensional conformal symmetry allows the computation of correlation functions of the so-called vertex operators, using bosonization techniques [33]. The same strategy was then applied to quantum spin chains once it became clear how to adapt the bosonization method to deformed commutation relations between creation and annihilation operators [34,35,36,37]. For the Heisenberg model, actual formal manipulations are made in the context of the equivalent six-vertex model where vertex operators are defined in the framework of the infinite-dimensional representation of the quantum group.…”
Section: Introductionmentioning
confidence: 99%