Stringy gravity, interacting tensionless strings and massless higher spins
By B. Sundborg. 2001
411 citations recorded by the source corpus.
Abstract Consequences of a strong version of the AdS/CFT correspondence for extremely stringy physics are examined. In particular, properties of N = 4 supersymmetric Yang-Mills theory are used to extract results about interacting tensionless strings and massless higher spin fields in an AdS5 × S5 background. Furthermore, the thermodynamics of this model signals the presence of a Hawking-Page phase transition between AdS5 space and a “black hole”-like high temperature configuration even in the extreme string limit.
Subfields: Astronomy and Astrophysics, Nuclear and High Energy Physics, Statistical and Nonlinear Physics
View Paper: https://www.semanticscholar.org/paper/ade536d7ab6e2ddca459273d68f9fdf44f103d4b
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Citations in the corpus
- On limits of superstring in AdS_5 x S^5 (2002, background): “tates corresponding to (5.25) and (5.30).p To conclude, we expect that the light-cone approach developed in [15, 5] and [2, 3] should be instrumental in proving the conjectured AdS/CFT correspondence [7, 8] in the λ→ 0 limit. Acknowledgments This work was supported in part by the DOE grant DE-FG02-9”
- Correlation functions of large N Chern-Simons-Matter theories and bosonization in three dimensions (2012, background): “Indeed, it was suggested in [5, 6] (see also [7, 8, 9]) that the bosonic theories are dual to the type A high-spin gravity theories of Vasiliev [10], and the fermionic theories to the type B high-spin gravity theories of Vasiliev.”
- Higher spins & strings (2014, background): “The AdS/CFT correspondence allows us to make this idea more concrete [6, 7, 8, 9].”
- Massless higher spins and holography (2002, background): “n the form of normal ordered products of single trace operators O(p i)ri and their derivatives, pi = 2,3,..., i= 1,...,n. For finite Nthere is mixing between the single-trace and multi-trace operators [7, 23]. This is because n-particle states in the bulk couple to operators that diagonalize the two-”
- Higher spin black holes (2011, background): “Introduction Theories of gravity coupled to massless higher spin fields [1,2,3,4,5] have received increased attention in recent years due to their appearance within the AdS/CFT correspondence [6,7,8,9,10,11,12,13,14,15,16,17,18,19,20,21].”
- Minimal model holography (2012, positive): “predictions from the bulk Vasiliev theory. Recall that this was the compelling piece of evidence [67, 68] for the Klebanov-Polyakov proposal for AdS4/CFT3 [90] and its generalisations [106], see also [109, 118, 97, 105] for earlier work. Below we will review the calculations [36, 4, 9, 37] that perf”
- Doubletons and 5D higher spin gauge theory (2001, background): “This implies AdS/CFT correspondence in a parameter regime where both boundary and bulk theories are perturbative.”
- Scalar fields and three-point functions in D = 3 higher spin gravity (2011, background): “For one, strings propagating in an AdS spacetime of string scale curvature are expected to be described by some theory of interacting higher spins [1,2,3]; while the precise theory remains unknown, the theories developed by Vasiliev and collaborators [4,5,6,7,8,9] appear to be, at the very least, so”
- AdS dual of the critical O(N) vector model (2002, methodology): “In particular, it was proposed that the massless higher-spin gauge theory with N = 8 supersymmetry in AdS5 is closely related to the free N = 4 large N SYM theory [11, 12, 15, 16, 18].”
- Conical defects in higher spin theories (2011, neutral): “[3, 4, 5, 6, 7, 8, 9, 1, 10]).”
- Spacetime geometry in higher spin gravity (2011, background): “Recently, theories with massless higher spin fields [4,5,6,7,8,9] have been reevaluated in the context of the gauge/gravity correspondence [10,11,12,13,14].”
- Partition functions of higher spin black holes and their CFT duals (2011, background): “Relatively recently, it has been realized that higher spin theories may lead to soluble examples of the AdS/CFT correspondence [3,4,5,6,7,8,9,10,11,12,13,14,15,16].”