Abstract

We consider the Wilson line networks of the Chern-Simons 3d gravity theory with toroidal boundary conditions which calculate global conformal blocks of degenerate quasi-primary operators in torus 2d CFT. After general discussion that summarizes and further extends results known in the literature we explicitly obtain the one-point torus block and two-point torus blocks through particular matrix elements of toroidal Wilson network operators in irreducible finite-dimensional representations of sl(2, ℝ) algebra. The resulting expressions are given in two alternative forms using different ways to treat multiple tensor products of sl(2, ℝ) representations: (1) 3mj Wigner symbols and intertwiners of higher valence, (2) totally symmetric tensor products of the fundamental sl(2, ℝ) representation.

Highlights

  • Conformal blocks are basic ingredients of conformal field theory correlation functions, they play crucial role in the conformal bootstrap program [1, 2]

  • After general discussion that summarizes and further extends results known in the literature we explicitly obtain the one-point torus block and two-point torus blocks through particular matrix elements of toroidal Wilson network operators in irreducible finite-dimensional representations of sl(2, R) algebra

  • There is an intriguing relation between the space of quantum states in the three-dimensional Chern-Simons theory in the presence of the Wilson lines and the space of conformal blocks in two-dimensional conformal field theory noticed a long ago [58,59,60]

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Summary

Introduction

Conformal blocks are basic ingredients of conformal field theory correlation functions, they play crucial role in the conformal bootstrap program [1, 2]. We formulate and calculate one-point and two-point Wilson network functionals which are dual to one-point and two-point torus conformal blocks for degenerate quasi-primary operators. — in section 3 we define toroidal Wilson network operators with one and two boundary attachments They are the basis for explicit calculations of one-point blocks and two-point blocks in two OPE channels . — in section 4 we consider torus conformal blocks for degenerate quasi-primary operators which are dual to the Wilson networks carrying finite-dimensional representations of the gauge algebra. — section 5 contains explicit calculation of the one-point toroidal Wilson network operator in two different representations, using 3j Wigner symbols and symmetric tensor product representation.

Wilson networks vs conformal blocks
Brief review of 3d Chern-Simons gravity theory
General construction
Vertex functions
Further developments
Toroidal Wilson networks
Global torus blocks
One-point blocks
Two-point blocks
Diagonal gauge
Wigner 3j symbol representation
Symmetric tensor product representation
Character decomposition
Two-point toroidal Wilson networks
Wigner 3j symbol representation of the s-channel block
Wigner 3j symbol representation of the t-channel block
Concluding remarks
C One-point block via Legendre functions
D Explicit examples of two-point Wilson network operators
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