Strings in flat space and pp waves from N = 4 Super Yang Mills

By D. Berenstein, J. Maldacena, H. Nastase. 2002

1,924 citations recorded by the source corpus.

Subfields: Artificial Intelligence, Nuclear and High Energy Physics

View Paper: https://www.semanticscholar.org/paper/8a9ac767a4ea0b62f31f876c676b39f4cba9a3e4

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Citations in the corpus

Exact anomalous dimensions of N=4 Yang-Mills operators with large R charge (2002, methodology): “It confirms the conjecture given in [5] and exactly coincides with the value obtained at strong coupling from the dual string approach [1].”
Stringing Spins and Spinning Strings (2003, background): “The first set of operators, belonging to the SO(6) representations [J, L − 2J, J ], interpolate smoothly between the BMN case of two impurities (J = 2) and the extreme case where the number of impurities equals half the total number of fields (J = L/2).”
Microscopic formulation of black holes in string theory (2002, background): “It is important to explore the consequences for the D1-D5 system, in particular to understand from the CFT the IIB string spectrum in the pp-wave limit of AdS3 × S(3) [224, 225].”
A semi-classical limit of the gauge/string correspondence (2002, methodology): “Our work is largely inspired by the recent important observation that, if the bare dimension of an operator becomes large simultaneously with λ, then the standard rule that the anomalous dimension blows up as λ may be violated [7, 8].”
Giant Gravitons - with Strings Attached (III) (2007, background): “3.1 Dynamical emergence of Chan-Paton factors 14 3.2 Physical basis 16”
T-systems and Y-systems in integrable systems (2010, background): “We do not intend to cover them here but refer to the literatures that will be cited in the next subsection and [179, 180, 181, 182, 183, 184, 185, 186, 187, 188, 189, 190, 191, 192] for example and references therein.”
Bethe ansatz for quantum strings (2004, background): “1 Separated Mode Numbers The direct quantization of string theory in the BMN limit [2] is feasible since the complicated curved background AdS5×S(5) may be replaced by the much simpler ppwave background.”
Three-dimensional N=6 SCFT's and their membrane dynamics (2008, background): “In the dual string world-sheet, this is the level matching constraint [52].”
Large spin limit of AdS5×S5 string theory and low energy expansion of ferromagnetic spin chains (2004, methodology): “1 Introduction Understanding AdS/CFT duality beyond the BPS or near BPS [1] limit remains an important challenge.”
Branes, anti-branes and Brauer algebras in gauge-gravity duality (2007, background): “Different multi-trace operators correspond to different states in the Hilbert space of N = 4 SYM on S(3) × R, via the operator-state correspondence (for elaboration of this see [7, 35, 36]).”
A relation between approaches to integrability in superconformal Yang-Mills theory (2003, methodology): “One development, which was stimulated by the BMN model of the plane wave limit of AdS5 × S(5) [8], has involved the study of the dilatation operator in perturbation theory.”
A Massive Study of M2-brane Proposals (2008, background): “In this case, for finite N , the field theory description (the plane-wave matrix model [44][45]) shows that the ground states are labeled simply by partitions of N , rather than labeled partitions.”
Wrapping interactions and a new source of corrections to the spin-chain/string duality (2005, background): “Non-trivial comparisons of gauge theory anomalous dimensions and string state energies can now be carried out in three different regimes: The BMN limit [13], the near BMN limit [14] and the spinning string limit [15].”
The Dilatation Operator of N=4 Super Yang-Mills Theory and Integrability (2004, methodology): “A simpler model which appears to have a lot in common with N = 4 SYM is the BMN matrix model [14].”
The quark anti-quark potential and the cusp anomalous dimension from a TBA equation (2012, neutral): “These insertions create a BMN vacuum [10].”