Abstract

We study the form factors of the Konishi operator, the prime example of non-protected operators in N=4 SYM theory, via the on-shell unitarity methods. Since the Konishi operator is not protected by supersymmetry, its form factors share many features with those in QCD, such as the occurrence of rational terms and of UV divergences that require renormalization. A subtle point is that this operator depends on the spacetime dimension. This requires a modification when calculating its form factors via unitarity methods. We derive a rigorous prescription that implements this modification to all loop orders and obtain the two-point form factor up to two-loop order and the three-point form factor to one-loop order. From these form factors, we construct an IR-finite cross section type quantity, namely the inclusive decay rate of the (off-shell) Konishi operator to any final (on-shell) state. Via the optical theorem, it is connected to the imaginary part of the two-point correlation function. We extract the Konishi anomalous dimension up to two-loop order from it.

Highlights

  • The framework of quantum field theories (QFTs) is very successful in describing the high-energy processes measured at colliders such as the LHC

  • We study the form factors of the Konishi operator, the prime example of nonprotected operators in N = 4 SYM theory, via the on-shell unitarity method

  • We have studied form factors of non-protected operators in N = 4 SYM theory, of the Konishi operator, using on-shell unitarity techniques

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Summary

Introduction

The framework of quantum field theories (QFTs) is very successful in describing the high-energy processes measured at colliders such as the LHC. We will see that the Konishi primary defined in (1.4) and involving a sum over the Nφ scalar field flavors depends on the dimension D, since Nφ = 10 − D is required to ensure supersymmetry This becomes important when regulating the divergences by continuing the theory from D = 4 to D = 4 − 2ǫ dimensions. We present the general strategy of computing the total cross section for a given operator using its form factors as building blocks. Since the Konishi operator is not protected, several interesting features appear in the results which have not occurred for amplitudes or BPS form factors in N = 4 SYM theory, e.g. UV divergences and rational terms.

Cross sections for two-point correlation functions in a nutshell
Renormalization of composite operators and their two-point functions
Two-point correlation functions and cross sections
Form factors for K6 via unitarity
Some BPS form factor results
Tree-level two- and three-point form factors
One-loop two-point form factor
Two-loop two-point form factor
One-loop three-point form factor
A subtlety in choosing a regularization scheme
From K6 to K
Final Konishi form factors
BPS and Konishi cross sections
BPS cross section up to one-loop order
Konishi cross section up to two-loop order
One-loop result
Two-loop result
Conclusion and outlook
A Fourier transformation of the two-point function
B Feynman integrals
C Passarino-Veltman reductions
D Checks of the three-point one-loop Konishi form factor
E Phase-space parametrization
F Anomalous dimensions via two-point form factors
G Renormalization-scheme transformations
H Feynman diagrams
Full Text
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