Spinning superstrings at two loops: strong-coupling corrections to dimensions of large-twist SYM operators
R. Roiban, A. A. Tseytlin
TL;DR
The authors compute the two-loop strong-coupling correction to the dimensions of large-twist SYM operators by analyzing a folded spinning string in AdS_5×S^5 with fixed charges in a semiclassical scaling limit. They develop a general framework using the world-sheet partition function with fixed E−S and J, perform a detailed sigma-model loop expansion around the classical solution, and extract energy corrections up to two loops. The results confirm the predicted leading log structure from the O(6) sigma-model and Alday–Maldacena, including matching coefficients for the ℓ^2 log ℓ and ℓ^2 log^2 ℓ terms, while highlighting the need to resum logarithms to interpolate to weak coupling. The work also sets up a systematic approach for higher-loop corrections and discusses the role of charge renormalization in shaping the strong-coupling expansion.
Abstract
We consider folded spinning strings in AdS_5xS^5 (with one spin component S in AdS_5 and J in S^5) corresponding to the Tr(D^S Z^J) operators in the sl(2) sector of the N=4 SYM theory in the special scaling limit in which both the string mass M ~ \sqrt λ\ln S and J are sent to infinity with their ratio fixed. Expanding in the parameter \el= J/M we compute the 2-loop string sigma model correction to the string energy and show that it agrees with the expression proposed by Alday and Maldacena in arxiv:0708.0672. We suggest that a resummation of the logarithmic \el^2 \ln^n \el terms is necessary in order to establish an interpolation to the weakly coupled gauge theory results. In the process, we set up a general framework for the calculation of higher loop corrections to the energy of multi-spin string configurations. In particular, we find that in addition to the direct 2-loop term in the string energy there is a contribution from lower loop order due to a finite ``renormalization'' of the relation between the parameters of the classical solution and the fixed spins, i.e. the charges of the SO(2,4) x SO(6) symmetry.
