Abstract

We study modular invariants arising in the four-point functions of the stress tensor multiplet operators of the mathcal{N} = 4 SU(N) super-Yang-Mills theory, in the limit where N is taken to be large while the complexified Yang-Mills coupling τ is held fixed. The specific four-point functions we consider are integrated correlators obtained by taking various combinations of four derivatives of the squashed sphere partition function of the mathcal{N} = 2∗ theory with respect to the squashing parameter b and mass parameter m, evaluated at the values b = 1 and m = 0 that correspond to the mathcal{N} = 4 theory on a round sphere. At each order in the 1/N expansion, these fourth derivatives are modular invariant functions of (τ, overline{tau} ). We present evidence that at half-integer orders in 1/N , these modular invariants are linear combinations of non-holomorphic Eisenstein series, while at integer orders in 1/N, they are certain “generalized Eisenstein series” which satisfy inhomogeneous Laplace eigenvalue equations on the hyperbolic plane. These results reproduce known features of the low-energy expansion of the four-graviton amplitude in type IIB superstring theory in ten-dimensional flat space and have interesting implications for the structure of the analogous expansion in AdS5× S5.

Highlights

  • One of the most intriguing features of four-dimensional gauge theories is the possibility of a mysterious duality that exchanges elementary quarks and magnetic monopoles, while relating physics at strong and weak gauge couplings

  • We study modular invariants arising in the four-point functions of the stress tensor multiplet operators of the N = 4 SU(N ) super-Yang-Mills theory, in the limit where N is taken to be large while the complexified Yang-Mills coupling τ is held fixed

  • Details of the perturbative sector of these functions are wellunderstood, we will not discuss the complete expressions for the instanton contributions in the Fourier expansion. Many details of these perturbative terms as well as the kinstanton/anti-instanton pairs have been determined and are presented in appendix C. This data will be compared with terms arising in the analysis of the localization formula for the SYM free energy, and provides compelling evidence that the 1/N 2 coefficient is proportional to a particular rational linear combination of the two modular invariants mentioned above

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Summary

Introduction

One of the most intriguing features of four-dimensional gauge theories is the possibility of a mysterious duality that exchanges elementary quarks and magnetic monopoles, while relating physics at strong and weak gauge couplings. Over the past twenty or so years, there have been steady developments on investigating the S-duality properties of N = 4 SYM using field theory methods, including numerous sophisticated checks based on supersymmetric partition functions [6, 11,12,13,14], extensions that incorporate supersymmetric defects [15,16,17,18,19,20], as well as refinements of the duality by keeping track of global structures of the gauge group and topological couplings in the theory [21,22,23].

Nq contributions with q
Overview of modular invariants and integrated correlators at large N
Sphere partition function from supersymmetric localization
Large N expansion of integrated correlators
Derivatives of deformed S4 partition function
Perturbative sector
Instanton sector
One-instanton sector
Two-instanton sector
Constraints from the flat space limit
Constraints from supersymmetric localization
Conclusion
A Scheme dependence and supersymmetric counter-terms
C Solutions of inhomogeneous Laplace equations
D Topological recursion
Details of perturbative calculation
Higher instanton sector
Details of instanton calculation
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