Abstract

A duality between the large N 't Hooft limit of the WD_N minimal model CFTs and a higher spin gravity theory on AdS3 is proposed. The gravity theory has massless spin fields of all even spins s=2,4,6,..., as well as two real scalar fields whose mass is determined by the 't Hooft parameter of the CFT. We show that, to leading order in the large N limit, the 1-loop partition function of the higher spin theory matches precisely with the CFT partition function.

Highlights

  • A duality between the large N ’t Hooft limit of the WDN minimal model CFTs and a higher spin gravity theory on AdS3 is proposed

  • To leading order in the large N limit, the 1-loop partition function of the higher spin theory matches precisely with the CFT partition function

  • The large N limit is taken while holding the ’t Hooft coupling λ fixed, where λ is to be identified with the parameter appearing in the commutation relations of the higher spin algebra

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Summary

The gravity partition function

Using the techniques of [24] the contribution of a massless spin s field to the 1-loop partition function on thermal AdS3 was found to be [23]. Combining the contributions from the fields of even spin s = 2, 4, 6, . . ., the higher spin part of the 1-loop partition function equals. The contribution of a real scalar field to the 1-loop partition function was determined in [25] (see [24]) to be. For h = h± as in (1.2) it was shown in [19] that the scalar 1-loop partition function can be written as. In the following we want to reproduce this partition function from the ’t Hooft limit of the coset CFTs (1.5)

The CFT analysis
The ’t Hooft limit
The branching functions
Matching the partition functions
Comments
The Weyl denominator formula
B The fusion calculation
Going up to level one
Full Text
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