Abstract:We show the factorization of the three-particle world-sheet S-matrix of AdS 5 ×S 5 superstring theory in the near-flat-space limit at one loop order. This is done by computing various scattering amplitudes from Feynman diagrams in the world-sheet theory. The knowledge of certain highest weight amplitudes allows us to fix all the freedom in the three-particle Smatrix, which we argue to be constrained up to four scalar functions due to the symmetries of the model. We demonstrate that these amplitudes are given b… Show more
“…Beyond the construction of the Lax connection much evidence has been accumulated for the integrability of the string also at the quantum level. Most relevant to our discussion here is the formulation of an exact worldsheet S-matrix [22][23][24][25][26][27][28][29][30][31][32][33][34][35][36][37][38][39][40] which matches with perturbative worldsheet calculations up to two loops in some cases [18,[41][42][43][44][45][46][47][48][49][50][51][52][53][54][55][56][57][58][59][60].…”
All symmetric space AdS n solutions of type II supergravity have recently been found for n > 2. For the supersymmetric solutions (and their T-duals) it is known that the Green-Schwarz string is classically integrable. We complete the classification by ruling out integrability for the remaining non-supersymmetric solutions. This is achieved by showing that tree-level scattering on the worldsheet of a GKP or BMN string fails to factorize for these cases.
“…Beyond the construction of the Lax connection much evidence has been accumulated for the integrability of the string also at the quantum level. Most relevant to our discussion here is the formulation of an exact worldsheet S-matrix [22][23][24][25][26][27][28][29][30][31][32][33][34][35][36][37][38][39][40] which matches with perturbative worldsheet calculations up to two loops in some cases [18,[41][42][43][44][45][46][47][48][49][50][51][52][53][54][55][56][57][58][59][60].…”
All symmetric space AdS n solutions of type II supergravity have recently been found for n > 2. For the supersymmetric solutions (and their T-duals) it is known that the Green-Schwarz string is classically integrable. We complete the classification by ruling out integrability for the remaining non-supersymmetric solutions. This is achieved by showing that tree-level scattering on the worldsheet of a GKP or BMN string fails to factorize for these cases.
“…We discuss the gauge-fixing and 3 In another kind of perturbative analysis of the worldsheet σ-model, i.e. the perturbative evaluation of the massive S-matrix for the elementary excitations around the BMN vacuum [44][45][46] (see also [15,47] for reviews), the one-loop computation for the full AdS5 × S 5 case [48][49][50] (in a certain regularization scheme) reproduces exactly the results [51] predicted by (symmetries and) quantum integrability. the decoupling of the longitudinal modes, as well as the arising of gauge connections in the covariant derivatives associated to the structure of normal bundle.…”
We discuss some geometrical aspects of the semiclassical quantization of string solutions in Type IIB Green-Schwarz action on AdS 5 × S 5 . We concentrate on quadratic fluctuations around classical configurations, expressing the relevant differential operators in terms of (intrinsic and extrinsic) invariants of the background geometry. The aim of our exercises is to present some compact expressions encoding the spectral properties of bosonic and fermionic fluctuations. The appearing of non-trivial structures on the relevant bundles and their role in concrete computations are also considered. We corroborate the presentation of general formulas by working out explicitly a couple of relevant examples, namely the spinning string and the latitude BPS Wilson loop.1
“…The scattering of the world-sheet excitations has been studied at tree-level in [7], while one-loop [8] and twoloop [9] results have been carried out only in the simpler near-flat-space limit [70] where interactions are at most quartic in the fields. These studies have also explicitly shown some consequences of the integrability of the model, such as the factorization of the many-body S-matrix and the absence of particle production in the scattering processes [71].…”