English

Form factors and the dilatation operator in $\mathcal{N}=4$ super Yang-Mills theory and its deformations

High Energy Physics - Theory 2016-03-04 v1

Abstract

In the first part of this thesis, we study form factors of general gauge-invariant local composite operators in N=4\mathcal{N}=4 super Yang-Mills theory at various loop orders and for various numbers of external legs. We show how to use on-shell methods for their calculation and in particular extract the dilatation operator from the result. We also investigate the properties of the corresponding remainder functions. Moreover, we extend on-shell diagrams, a Gra{\ss}mannian integral formulation and an integrability-based construction via R-operators to form factors, focussing on the chiral part of the stress-tensor supermultiplet as an example. In the second part, we study the β\beta- and the γi\gamma_i-deformation, which were respectively shown to be the most general supersymmetric and non-supersymmetric field-theory deformations of N=4\mathcal{N}=4 super Yang-Mills theory that are integrable at the level of the asymptotic Bethe ansatz. For these theories, a new kind of finite-size effect occurs, which we call prewrapping and which emerges from double-trace structures that are required in the deformed Lagrangians. While the β\beta-deformation is conformal when the double-trace couplings are at their non-trivial IR fixed points, the γi\gamma_i-deformation has running double-trace couplings without fixed points, which break conformal invariance even in the planar theory. Nevertheless, the γi\gamma_i-deformation allows for highly non-trivial field-theoretic tests of integrability at arbitrarily high loop orders.

Keywords

Cite

@article{arxiv.1603.01145,
  title  = {Form factors and the dilatation operator in $\mathcal{N}=4$ super Yang-Mills theory and its deformations},
  author = {Matthias Wilhelm},
  journal= {arXiv preprint arXiv:1603.01145},
  year   = {2016}
}

Comments

175 pages, PhD thesis based on the author's publications arXiv:1308.4420, arXiv:1312.2959, arXiv:1405.6712, arXiv:1410.6309, arXiv:1410.8485, arXiv:1504.06323 and arXiv:1506.08192