2000
DOI: 10.1007/pl00005536
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and as Vertex Operator Extensions¶of Dual Affine Algebras

Abstract: Abstract. We discover a realisation of the affine Lie superalgebra sℓ(2|1) and of the exceptional affine superalgebra D(2|1; α) as vertex operator extensions of two sℓ(2) algebras with 'dual ' levels (and an auxiliary level-1 sℓ(2) algebra). The duality relation between the levels is (k 1 +1)(k 2 +1) = 1. We construct the representation of sℓ(2|1) k1 on a sum of tensor products of sℓ(2) k1 , sℓ(2) k2 , and sℓ(2) 1 modules and decompose it into a direct sum over the sℓ(2|1) k1 spectral flow orbit. This decompos… Show more

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Cited by 33 publications
(38 citation statements)
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“…The ;θ notation is for the spectral flow transform, see (B.5) [13,33]. The four different sectors (Ramond, Neveu-Schwarz, super-Ramond, and super-Neveu-Schwarz) are mapped under the S and T transformations as indicated in (B.35).…”
Section: Formulation Of the Main Resultmentioning
confidence: 99%
See 1 more Smart Citation
“…The ;θ notation is for the spectral flow transform, see (B.5) [13,33]. The four different sectors (Ramond, Neveu-Schwarz, super-Ramond, and super-Neveu-Schwarz) are mapped under the S and T transformations as indicated in (B.35).…”
Section: Formulation Of the Main Resultmentioning
confidence: 99%
“…Admissible sℓ(2|1) representations L r,s,ℓ,u;θ . The admissible sℓ(2|1)-representations, which belong to the class of irreducible highest-weight representations characterized by the property that the corresponding Verma modules are maximal elements with respect to the (appropriately defined) Bruhat order, have arisen in a vertex-operator extension of two sℓ(2) algebras with the "dual" levels k and k ′ such that (k + 1)(k ′ + 1) = 1 [33]; via this extension sℓ(2) k ⊕ sℓ(2) k ′ → sℓ(2|1) k , the admissible sℓ(2|1) representations are related to the admissible sℓ(2) representations [45]. We fix the sℓ(2|1) level as k = ℓ u − 1 with coprime positive integers ℓ and u.…”
Section: Discussionmentioning
confidence: 99%
“…Since these states generate relaxed highest-weight modules in which the charged singular vector generates exactly the identity module, their irreducible module 13 χ R ⋆ µ1,µ2;θ (z, q) will not 12 There is a minor difference in the picture provided in [3], as the L 0 direction is inverted in that paper. 13 Here we really consider the irreducible modules R ⋆ from which the charged singular vector has been factored out.…”
Section: The I 0 Charactermentioning
confidence: 99%
“…This "duality" between two levels, k and p − 1, was extensively used in [39,40] (see also the references therein); in particular,…”
Section: (57(4)mentioning
confidence: 99%