Integrability of two-loop dilatation operator in gauge theories
A.V. Belitsky, G.P. Korchemsky, D. M\"uller

TL;DR
This paper investigates the two-loop dilatation operator in various gauge theories, revealing that integrability persists at two loops in the planar limit despite conformal symmetry breaking, but is broken by nonplanar effects in QCD.
Contribution
It demonstrates that integrability of the two-loop dilatation operator survives conformal symmetry breaking in certain gauge theories and clarifies its dependence on planarity and supersymmetry.
Findings
Integrability persists at two loops in the planar limit of these gauge theories.
Nonplanar diagrams in QCD break the integrability at two loops.
In SYM theories, the two-loop dilatation operator's spectrum is similar across different models.
Abstract
We study the two-loop dilatation operator in the noncompact SL(2) sector of QCD and supersymmetric Yang-Mills theories with N=1,2,4 supercharges. The analysis is performed for Wilson operators built from three quark/gaugino fields of the same helicity belonging to the fundamental/adjoint representation of the SU(3)/SU(N_c) gauge group and involving an arbitrary number of covariant derivatives projected onto the light-cone. To one-loop order, the dilatation operator inherits the conformal symmetry of the classical theory and is given in the multi-color limit by a local Hamiltonian of the Heisenberg magnet with the spin operators being generators of the collinear subgroup of full (super)conformal group. Starting from two loops, the dilatation operator depends on the representation of the gauge group and, in addition, receives corrections stemming from the violation of the conformal…
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