2010
DOI: 10.1103/physrevd.82.045016
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Symmetries of tree-level scattering amplitudes inN=6superconformal Chern-Simons theory

Abstract: Constraints of the osp(6|4) symmetry on tree-level scattering amplitudes in N = 6 superconformal Chern-Simons theory are derived. Supplemented by Feynman diagram calculations, solutions to these constraints, namely the four-and six-point superamplitudes, are presented and shown to be invariant under Yangian symmetry. This introduces integrability into the amplitude sector of the theory.

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Cited by 96 publications
(222 citation statements)
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References 66 publications
(104 reference statements)
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“…This results in SUSY invariants that contain different degree of Grassmann polynomials, which are difficult to analyze. One can instead use R-symmetry decomposition instead much like the x ± variables introduced in three-dimensions [37]. Explicit solutions for these projection variables at higher points may reveal new protected sectors.…”
Section: Jhep09(2015)098mentioning
confidence: 99%
See 1 more Smart Citation
“…This results in SUSY invariants that contain different degree of Grassmann polynomials, which are difficult to analyze. One can instead use R-symmetry decomposition instead much like the x ± variables introduced in three-dimensions [37]. Explicit solutions for these projection variables at higher points may reveal new protected sectors.…”
Section: Jhep09(2015)098mentioning
confidence: 99%
“…It is rather non-trivial to check that it vanishes under the multiplicative R-symmetry generators. To simplify our task, we will follow [37] and project the fermionic variables η i on a convenient basis.…”
Section: Jhep09(2015)098mentioning
confidence: 99%
“…Using the notation that the fundamental and anti-fundamental indices of SU(N 1 ) and SU(N 2 ) are given by ( α , α ) and (α,α) respectively, the color dressed amplitude of k matter states (Φ i )α α and k anti-matter states (Φ i ) αα , with n = 2k, is conveniently decomposed as [38] A…”
Section: Jhep11(2013)050mentioning
confidence: 99%
“…The holomorphic o(2N+2) currents are generated by the dimension one currents ψ i ψ j , the sp(2N) currents are generated by the β a β b , γ a β b and γ a γ b and the fermionic currents are of the form ψ i β a and ψ i γ a . This realisation is the affine analogue of an oszillator realisation for the horizontal subsuperalgebra for which the vanishing of the righthand side of the Serre relations is understood [58]. The current-current perturbation field O GN = J a κ baJ b transforms in the adjoint representation under both holomorphic and anti-holomorphic currents.…”
Section: (44)mentioning
confidence: 99%