The Bethe ansatz for superconformal Chern-Simons
By J. Minahan, K. Zarembo. 2008
359 citations recorded by the source corpus.
We study the anomalous dimensions for scalar operators for a three-dimensional Chern-Simons theory recently proposed in arXiv:0806.1218. We show that the mixing matrix at two-loop order is that for an integrable Hamiltonian of an SU(4) spin chain with sites alternating between the fundamental and the anti-fundamental representations. We find a set of Bethe equations from which the anomalous dimensions can be determined and give a proposal for the Bethe equations to the full superconformal group of OSp(2,2|6).
Subfields: Atomic and Molecular Physics, and Optics, Geometry and Topology, Nuclear and High Energy Physics
View Paper: https://www.semanticscholar.org/paper/b1a5874ffa4a015d38f6c633d4d2277927b99df6
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In Atomic and Molecular Physics, and Optics
- A. Tseytlin
- S. Frolov
- R. Roiban
- G. Arutyunov
- Alessandro Sfondrini
- L. Alday
- Tristan McLoughlin
- K. Hosomichi
In Geometry and Topology
- S. Frolov
- G. Arutyunov
- Alessandro Sfondrini
- A. Tseytlin
- R. Roiban
- L. Alday
- Diego Trancanelli
- Tristan McLoughlin
In Nuclear and High Energy Physics
Citations in the corpus
- N = 6 super Chern-Simons theory S-matrix and all-loop Bethe ansatz equations (2008, background): “) The integrability of the planar N = 6 CS was first discovered by Minahan and Zarembo [8] in the leading two-loop-order perturbative computation of the anomalous dimensions of gauge-invariant composite operators.”
- Three-dimensional N=6 SCFT's and their membrane dynamics (2008, methodology): “A notable feature of the string theory limit of the ABJM theory, whose sigma model was studied in [14, 15] and, using a covariant formulation, in [16], is that it appears to be integrable [17, 18] (see also [19, 20]).”
- Spinning strings at one-loop in AdS(4) x P**3 (2008, methodology): “The dilatation operator of the N = 6 Chern-Simons theory was shown [16, 18], to leading order in the scalar sector, to be equivalent to the Hamiltonian of an integrable (alternating) spin chain.”
- Anomalous radius shift in AdS4/CFT3 (2009, background): “At large N and k the theory has an ’tHooft (planar) limit with fixed λ ≡ N/k, and the field theory description is (perturbatively) valid when λ≪ 1, i.e. for k ≫ N .”
- Semiclassical quantization of spinning strings in AdS4 × ℂℙ3 (2008, background): “Complementary, the planar superconformal Chern-Simons theory appears to be integrable at leading order in the weak coupling expansion [8, 9, 10].”
- Quantum spinning strings in AdS_4 x CP^3: testing the Bethe Ansatz proposal (2008, background): “This is for a good reason, as both the perturbative gauge theory and the dual free string theory appear to be integrable (as was partially verified at two-loop level in gauge theory – namely in the scalar sector [2] – and at the classical level in string theory [3, 4]).”
- Towards integrability for AdS 3 / CFT 2 ?> (2014, background): “Integrability manifests itself in the ABJM theory, where an integrable spin-chain Hamiltonian was found first at two loop in perturbation theory [143, 144].”
- Spin Chains in N = 6 Superconformal Chern-Simons-Matter Theory (2008, methodology): “Note added in proof: Upon completion of the bulk of this work, we received [19] and [16], which contain results that overlap with different parts of this paper.”
- Superstrings on AdS4 × ℂℙ3 as a coset sigma-model (2008, background): “in the weak coupling expansion the corresponding dilatation operator can be identified with an integrable Hamiltonian of the SU(4) spin chain with spins alternating between fundamental and anti-fundamental representations [4].”
- N=5,6 Superconformal Chern-Simons Theories and M2-branes on Orbifolds (2008, background): “The relevant topics include extension to N = 4 orbifolds [27, 28], superconformal indices [29], Penrose limit [30], integrability [31], non-supersymmetric generalization [32], and partition function [16].”
- Integrability, spin-chains and the AdS3/CFT2 correspondence (2011, positive): “Restricting to just one osp(4|2) factor the spin-chain we construct is closely related to the ABJM spin-chain constructed in [57].”