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
Summary
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.
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