In this paper we consider the collective field theory description of the singlet sector of a free matrix field in 2+1 dimensions. This necessarily involves the study of k-local collective fields, which are functions of $2k+1$ coordinates. We argue that these coordinates have a natural interpretation: the k-local collective field is a field defined on an AdS₄×Sᵏ⁻²×Sᵏ⁻¹ spacetime. The modes of a harmonic expansion on the Sᵏ⁻²×Sᵏ⁻¹ portion of the spacetime leads to the spinning bulk fields of the dual gravity theory.
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Koch et al. (2024) studied this question.
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