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Chern-Simons vector models and higher spins - Ginzburg ...

Chern-Simons vector models and higher spins - Ginzburg ...

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<strong>Chern</strong>-<strong>Simons</strong> <strong>vector</strong> modelS = k ∫4π S CS(A) + d 3 x ¯ψ i γ µ D µ ψ i i = 1, . . . , NWe will be interested in the large N ’t Hooft limitN → ∞, k → ∞ with λ = N k fixedIn this limit, we effectively have a continuous line of non-susy CFT’sparameterized by λ. At λ = 0 we reduce to the free fermionic <strong>vector</strong>model.All I said so far applies for fermion being in any representation, e.g.the adjoint. However, working with a <strong>vector</strong> fermion entails severalsimplifications so that exact results become possible.The analogous <strong>Chern</strong>-<strong>Simons</strong> bosonic <strong>vector</strong> model has been studiedin parallel to our work in Aharony et. al., 2011. Also, interesting workin progress on susy extensions of these <strong>Chern</strong>-<strong>Simons</strong> <strong>vector</strong> <strong>models</strong>(see X. Yin talk).Simone Giombi (PI) <strong>Chern</strong>-<strong>Simons</strong> <strong>and</strong> <strong>higher</strong> <strong>spins</strong> Lebedev Inst., Jun 1 2012 10 / 24

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