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<p>Planar parts of conformal dimensions of primary operators in <i>U</i><sub><i>k</i></sub>(<i>N</i>) × <i>U</i><sub>−<i>k</i></sub>(<i>N</i>) ABJM theory are controlled by integrability. Strong coupling asymptotics of planar dimensions of operators with large spins can be found from the energy of semiclassical strings in AdS<sub>4</sub> × CP<sup>3</sup> but computing non-planar corrections requires understanding higher genus string corrections. As was pointed out in arXiv:2408.10070, there is an alternative way to find the non-planar corrections by quantizing M2 branes in AdS<sub>4</sub> × <i>S</i><sup>7</sup>/ℤ<sub><i>k</i></sub> which are wrapped around the 11d circle of radius 1/<i>k</i> = <i>λ/N</i> and generalize spinning strings in AdS<sub>4</sub> × CP<sup>3</sup>. Computing the 1-loop correction to the energy of M2 brane that corresponds to the long folded string with large spin <i>S</i> in AdS<sub>4</sub> allowed to obtain a prediction for the large <i>λ</i> limit of non-planar corrections to the cusp anomalous dimension. Similar predictions were found for non-planar dimensions of operators dual to M2 branes that generalize the “short” and “long” circular strings with two equal spins <i>J</i><sub>1</sub> = <i>J</i><sub>2</sub> in CP<sup>3</sup>. Here we consider two more non-trivial examples of 1-loop M2 brane computations that correspond to: (i) long folded string with large spin <i>S</i> in AdS<sub>4</sub> and orbital momentum <i>J</i> in CP<sup>3</sup> whose energy determines the generalized cusp anomalous dimension, and (ii) circular string with spin <i>S</i> in AdS<sub>4</sub> and spin <i>J</i> in CP<sup>3</sup>. We find the leading terms of the expansion of the corresponding 1-loop M2 brane energies in 1/<i>k</i>. We also discuss similar semiclassical 1-loop M2 brane computation in flat 11d background and comment on possible relation to higher genus corrections to energies in 10d string theory.</p>

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On non-planar ABJM anomalous dimensions from M2 branes in AdS4 × S7/ℤk

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  • 发表日期：

    2025年5月21日

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  • Matteo Beccaria,
  • Stefan A. Kurlyand,
  • Arkady A. Tseytlin

摘要

Planar parts of conformal dimensions of primary operators in Uk(N) × U−k(N) ABJM theory are controlled by integrability. Strong coupling asymptotics of planar dimensions of operators with large spins can be found from the energy of semiclassical strings in AdS4 × CP3 but computing non-planar corrections requires understanding higher genus string corrections. As was pointed out in arXiv:2408.10070, there is an alternative way to find the non-planar corrections by quantizing M2 branes in AdS4 × S7/ℤk which are wrapped around the 11d circle of radius 1/k = λ/N and generalize spinning strings in AdS4 × CP3. Computing the 1-loop correction to the energy of M2 brane that corresponds to the long folded string with large spin S in AdS4 allowed to obtain a prediction for the large λ limit of non-planar corrections to the cusp anomalous dimension. Similar predictions were found for non-planar dimensions of operators dual to M2 branes that generalize the “short” and “long” circular strings with two equal spins J1 = J2 in CP3. Here we consider two more non-trivial examples of 1-loop M2 brane computations that correspond to: (i) long folded string with large spin S in AdS4 and orbital momentum J in CP3 whose energy determines the generalized cusp anomalous dimension, and (ii) circular string with spin S in AdS4 and spin J in CP3. We find the leading terms of the expansion of the corresponding 1-loop M2 brane energies in 1/k. We also discuss similar semiclassical 1-loop M2 brane computation in flat 11d background and comment on possible relation to higher genus corrections to energies in 10d string theory.