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BFKL pomeron in the next-to-next-to-leading approximation in the planar N=4 SYM theory

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arxiv 1508.02857 v1 pith:I2YQY3O4 submitted 2015-08-12 hep-th hep-exhep-ph

BFKL pomeron in the next-to-next-to-leading approximation in the planar N=4 SYM theory

classification hep-th hep-exhep-ph
keywords approximationbfklnext-to-next-to-leadingplanartheoryanomalouscomingconstraints
verification ladder T0 review T1 audit T2 compute T3 formal T4 reserved
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We find the eigenvalue of the kernel of BFKL equation in the next-to-next-to-leading logarithm approximation in the planar N=4 SM theory from the constraints, coming from the six-loop anomalous dimension of twist-2 operators and known large-gamma limit.

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Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score.

  1. The next-to-next-to-leading order BFKL eigenvalue at odd conformal spin in planar N=4 super Yang-Mills: closed form, coefficient structure, and arithmetic

    hep-th 2026-07 conditional novelty 8.0

    The NNLO BFKL eigenvalue of planar N=4 SYM is given in closed form at every odd conformal spin via exact Mellin extraction from the Caron-Huot–Herranen integrand, matching quantum spectral curve intercepts through n=91.

  2. The next-to-next-to-leading order BFKL eigenvalue at odd conformal spin in planar N=4 super Yang-Mills

    hep-th 2026-07 conditional novelty 7.0

    The NNLO BFKL eigenvalue of planar N=4 SYM is now in closed form at every odd spin n, with ν=0 intercepts matching Quantum Spectral Curve data through n=91.