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Three-point functions in the SU(2) sector at strong coupling

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arxiv 1312.3727 v2 pith:YYTJD5KG submitted 2013-12-13 hep-th

classification hep-th
keywords three-pointcouplingfunctionsarxivcontoursintegrationsectorstates
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abstract

Extending the methods developed in our previous works (arXiv:1110.3949, arXiv:1205.6060), we compute the three-point functions at strong coupling of the non-BPS states with large quantum numbers corresponding to the composite operators belonging to the so-called SU(2) sector in the $\mathcal{N}=4$ super-Yang-Mills theory in four dimensions. This is achieved by the semi-classical evaluation of the three-point functions in the dual string theory in the $AdS_3 \times S^3$ spacetime, using the general one-cut finite gap solutions as the external states. In spite of the complexity of the contributions from various parts in the intermediate stages, the final answer for the three-point function takes a remarkably simple form, exhibiting the structure reminiscent of the one obtained at weak coupling. In particular, in the Frolov-Tseytlin limit the result is expressed in terms of markedly similar integrals, however with different contours of integration. We discuss a natural mechanism for introducing additional singularities on the worldsheet without affecting the infinite number of conserved charges, which can modify the contours of integration.

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Cited by 2 Pith papers

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    In planar N=4 SYM, the large-spin OPE coefficient for two maximal giant gravitons and a twist-two operator scales as S^{d(g)}, with d(g) computed at arbitrary coupling.

  2. Liouville Theory, AdS$_2$ String, and Three-Point Functions

    hep-th 2019-08 conditional novelty 3.0 of 10

    Classical three-point functions in Liouville theory and for AdS2 strings can be derived from ODE/IM-style functional equations, with the Liouville result matching the DOZZ formula and the AdS2 result expressed through...

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