Abstract
The mathcal{N} = 4 higher spin generators for general superspin s in terms of oscillators in the matrix generalization of AdS3 Vasiliev higher spin theory at nonzero μ (which is equivalent to the ’t Hooft-like coupling constant λ) were found previously. In this paper, by computing the (anti)commutators between these mathcal{N} = 4 higher spin generators for low spins s1 and s2 (s1 + s2 ≤ 11) explicitly, we determine the complete mathcal{N} = 4 higher spin algebra for generic μ. The three kinds of structure constants contain the linear combination of two different generalized hypergeometric functions. These structure constants remain the same under the transformation μ ↔ (1 − μ) up to signs. We have checked that the above mathcal{N} = 4 higher spin algebra contains the mathcal{N} = 2 higher spin algebra, as a subalgebra, found by Fradkin and Linetsky some time ago.
Highlights
It is known that there exists a large N = 4 holography [1] which connects the matrix generalization of the Vasiliev higher spin theory [2, 3] on AdS3 with the two dimensional minimal model conformal field theories having the large N = 4 superconformal symmetry
AdS3 bulk theory corresponds to the free parameter of the large N = 4 superconformal algebra. The former is related to the mass of the scalar field while the latter is given by a particular combination of N and a level k in the N = 4 unitary coset model
We have considered 2 × 2 matrix generalization of AdS3 Vasiliev higher spin theory
Summary
How to obtain the N = 2 higher spin algebra shs[λ] from N = 4 higher spin algebra shs2[λ]. The (anti)commutators of oscillators by using the structure constants in shs[μ] 55. F.3.1 The structure constants in the shs[μ] by using the generalized hypergeometric functions. F.3.2 The relations between the structure constants in the shs2[μ] and those in the shs[μ]
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