Chern Simons duality with a fundamental boson and fermion
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In this paper, the thermal free energy for all renormalizable Chern Simon the-Ories coupled to a single fundamental bosonic and fermionic field in the T Hooft large N limit was derived.Abstract:
We compute the thermal free energy for all renormalizable Chern Simon the- ories coupled to a single fundamental bosonic and fermionic field in the 't Hooft large N limit. We use our results to conjecture a strong weak coupling duality invariance for this class of theories. Our conjectured duality reduces to Giveon Kutasov duality when restricted to N = 2 supersymmetric theories and to an earlier conjectured bosonization duality in an appropriate decoupling limit. Consequently the bosonization duality may be regarded as a deformation of Giveon Kutasov duality, suggesting that it is true even at large but finite N.read more
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Time-Reversal Breaking in QCD$_4$, Walls, and Dualities in 2+1 Dimensions
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References
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Quantum field theory and the Jones polynomial
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Constraining conformal field theories with a higher spin symmetry
TL;DR: In this article, the authors studied the constraints imposed by the existence of a single higher spin conserved current on a three-dimensional conformal field theory and showed that the correlation functions of the stress tensor and the conserved currents are equal to those of a free field theory.
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d = 3 bosonic vector models coupled to Chern-Simons gauge theories
TL;DR: In this paper, the authors studied three-dimensional O(N) (U(N)) vector models with the Chern-Simons theory coupled to a scalar field in the fundamental representation, in the large N limit.
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Chern–Simons theory with vector fermion matter
Simone Giombi,Shiraz Minwalla,Shiroman Prakash,Sandip P. Trivedi,Spenta R. Wadia,Spenta R. Wadia,Xi Yin +6 more
TL;DR: In this paper, the authors study three-dimensional conformal field theories described by U(N) Chern-Simons theory at level k coupled to massless fermions in the fundamental representation and compute the exact planar free energy of the theory at finite temperature on ℝ2 as a function of the ’t-Hooft coupling λ=N/k.