Abstract

We compute two-loop form factors of operators in the $SU(2|3)$ closed subsector of $N=4$ supersymmetric Yang-Mills. In particular, we focus on the non-protected, dimension-three operators $\mathrm{Tr} (X[Y,Z])$ and $\mathrm{Tr} ( \psi \psi)$ for which we compute the four possible two-loop form factors, and corresponding remainder functions, with external states $\langle \bar{X} \bar{Y} \bar{Z}|$ and $\langle \bar{\psi} \bar{\psi}|$. Interestingly, the maximally transcendental part of the two-loop remainder of $\langle\bar{X} \bar{Y} \bar{Z}| \mathrm{Tr} (X[Y,Z]) |0\rangle$ turns out to be identical to that of the corresponding known quantity for the half-BPS operator $\mathrm{Tr} (X^3)$. We also find a surprising connection between the terms subleading in transcendentality and certain a priori unrelated remainder densities introduced in the study of the spin chain Hamiltonian in the SU(2) sector. Next, we use our calculation to resolve the mixing, recovering anomalous dimensions and eigenstates of the dilatation operator in the SU(2|3) sector at two loops. We also speculate on potential connections between our calculations in $N=4$ super Yang-Mills and Higgs + multi-gluon amplitudes in QCD in an effective Lagrangian approach.

Highlights

  • The study of form factors of composite operators is a very active area of research

  • It is interesting that they appear in the larger SU(2|3) sector, possibly pointing to some universality of these quantities. This finding leads us to speculate that the leading transcendental part of the correction terms to Higgs + multi-gluon processes induced by the interactions Oi, i ≥ 1, on the right-hand side of (1.2), can be equivalently obtained by computing their form factors in the much simpler N = 4 supersymmetric Yang-Mills (SYM) theory

  • R-symmetry allows for two possibilities for the particles running in the loop, namely two scalars and a gluon, or two fermions and a scalar

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Summary

Introduction

The study of form factors of composite operators is a very active area of research. After the pioneering paper [1], interest in the calculation of form factors in supersymmetric theories was rekindled at strong coupling in [2] and at weak coupling in [3]. Operators OB and OF for which we compute the four possible two-loop form factors, and corresponding remainder functions with external states X Y Z| and ψψ| It is convenient, and natural from the point of view of operator mixing discussed later, to package them into a matrix of form factors: ψψ|OF |0. It is interesting that they appear (in some form) in the larger SU(2|3) sector, possibly pointing to some universality of these quantities This finding leads us to speculate that the leading transcendental part of the correction terms to Higgs + multi-gluon processes induced by the interactions Oi, i ≥ 1, on the right-hand side of (1.2), can be equivalently obtained by computing their form factors (or form factors related by supersymmetry) in the much simpler N = 4 SYM theory. Often we will use the following shorthand notation if labels are not needed, in particular X Y Z| := 1φ12 2φ23 3φ31 | and ψψ| := 1ψ123 2ψ123 |

A useful decomposition
Two-particle cuts and result
Auxiliary one-loop form factors needed for two-loop cuts
Three-particle cuts of the two-loop form factor
Three-particle cuts in the s23-channel
Summary and integral reduction
Definition of the remainder
Two-particle cut in the q2-channel
Two-particle cut in the s23-channel
Final result
Conclusions
A One-loop integral functions
B Comparing half-BPS form factors

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