Fivebranes from gauge theory
By Hai Lin, J. Maldacena. 2005
214 citations recorded by the source corpus.
We study theories with 16 supercharges and a discrete energy spectrum. One class of theories has symmetry group SU(2|4). They arise as truncations of N=4 super Yang-Mills theory. They include the plane-wave matrix model, 2+1 super Yang-Mills theory on RxS{sup 2} and N=4 super Yang-Mills theory on RxS{sup 3}/Z{sub k}. We explain how to obtain their gravity duals in a unified way. We explore the regions of the geometry that are relevant for the study of some 1/2 BPS and near BPS states. This leads to a class of two dimensional (4,4) supersymmetric sigma models with nonzero H flux, including a massive deformed WZW model. We show how to match some features of the string spectrum with the Yang-Mills theory. The other class of theories are also connected to N=4 super Yang-Mills theory and arise by making some of the transverse scalars compact. Their vacua are characterized by a 2D Yang-Mills theory or 3D Chern-Simons theory. These theories realize peculiar super-Poincare symmetry algebras in 2+1 or 1+1 dimensions with ''noncentral'' charges. We finally discuss gravity duals of N=4 super Yang-Mills theory on AdS{sub 3}xS{sup 1}.
Subfields: Astronomy and Astrophysics, Nuclear and High Energy Physics
View Paper: https://www.semanticscholar.org/paper/fa52aabff1021c40c676f50705364673ebcc7cbd
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Citations in the corpus
- N=6 superconformal Chern-Simons-matter theories, M2-branes and their gravity duals (2008, methodology): “uperpotential (which is just (2.3) for this special case) W= 2π k Tr(AiBiAjBj− BiAiBjAj) = 4π k Tr(A 1B 1A 2B 2 − A 1B 2A 2B 1). (2.5) 3 Theories with N = 4 but a modified superalgebra were written in [17]. 5 As described above, we can obtain this theory by starting from the 2 + 1 dimensional N = 4 g”
- On gravitational description of Wilson lines (2006, background): “(11)It is interesting to observe that the boundary conditions on surfaces similar to ones depicted in figure 3b were encountered in a description of BPS geometries in M theory [24].”
- Three-dimensional N=6 SCFT's and their membrane dynamics (2008, background): “12 This same renormalization is responsible for the complicated boundary conditions that one finds in Mtheory bubbling geometries [92].”
- An Index for 4 Dimensional Super Conformal Theories (2005, methodology): “The representation theory of this group was studied in [22,23] and the index was used in [24] to analyze various field theories with this symmetry.”
- Rigid Surface Operators (2008, background): “Following [26, 27], we call these bubbling geometries.”
- On type IIA Penrose limit and = 6 Chern-Simons theories (2008, result): “We will also notice that in the ABJM theory, we can define a BMN-like operator and we will compute its anomalous dimension to leading order of the effective (3)The same plane-wave also appears in the study of the gravity dual of a 2+1 super Yang-Mills with SU(2|4) symmetry [50], where the string spe”
- Deformations of superconformal theories (2016, background): “To see this, we follow [52] and consider a massless particle with lightcone momentum P+ = E and P− = P3 = 0, on which (4.”
- The su(2|2) dynamic S-matrix (2005, background): “In theexcitation picturethism ightappearnotto be a problem as the num ber ofexcitations is preserved,but even there one nds avour uctuationswhich m ay appearproblem atic[13].”
- 4d Index to 3d Index and 2d TQFT (2011, background): “Here L(p, q), where p, q are coprime (1)The index of N = 4 super-Yang-Mills on S(1) × S(3)/Zp was studied in [16, 17].”
- Spin Chains in N = 6 Superconformal Chern-Simons-Matter Theory (2008, background): “A similar phenomenon was observed in [29].”
- SUPERCONFORMAL FIELD THEORIES (2005, unknown): “Similarly one can use the (1)In the course of this work related work has been published [6].”
- A Massive Study of M2-brane Proposals (2008, background): “[48] for the explicit form of the algebra.”