2019
DOI: 10.1007/jhep12(2019)043
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Chern-Simons dualities with multiple flavors at large N

Abstract: We study U (N ) k Chern-Simons theory coupled to fundamental fermions and scalars in a large N 't Hooft limit. We compute the thermal free energy at high temperature, as well as two-and three-point functions of simple gauge-invariant operators. Our findings support various dualities between Chern-Simons-matter theories with N = 0, 1, and 2 supersymmetry.1 When either N f or Ns = 0, i.e. when we have Chern-Simons theory coupled to purely scalar or fermion matter, there is evidence [36] for a different dual desc… Show more

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Cited by 9 publications
(3 citation statements)
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References 57 publications
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“…The off-shell free energy is a quantity that depends on some auxiliary variables in addition to the UV parameters of the theory, the temperature, chemical potential and eigenvalue distribution ρ. It turns out that once we perform the path integral (3.3) via saddle point approximation and obtain an answer for v [ρ] at each of the various large N saddle points, the whole procedure can be replaced by a simpler one: that of performing an ordinary integral over a few auxiliary variables, denoted collectively as ϕ aux , with the integrand being a function of these variables rather than being a functional of fields: 73,80] and F (ϕ aux ; ρ] in the presence of chemical potential were carefully computed only for values of the chemical potential smaller than the thermal masses of the bosonic or fermionic excitations in the respective theories. We present these expressions for the free energy in the next subsection.…”
Section: The Off-shell Free Energymentioning
confidence: 99%
“…The off-shell free energy is a quantity that depends on some auxiliary variables in addition to the UV parameters of the theory, the temperature, chemical potential and eigenvalue distribution ρ. It turns out that once we perform the path integral (3.3) via saddle point approximation and obtain an answer for v [ρ] at each of the various large N saddle points, the whole procedure can be replaced by a simpler one: that of performing an ordinary integral over a few auxiliary variables, denoted collectively as ϕ aux , with the integrand being a function of these variables rather than being a functional of fields: 73,80] and F (ϕ aux ; ρ] in the presence of chemical potential were carefully computed only for values of the chemical potential smaller than the thermal masses of the bosonic or fermionic excitations in the respective theories. We present these expressions for the free energy in the next subsection.…”
Section: The Off-shell Free Energymentioning
confidence: 99%
“…This duality is embedded within a larger duality web [15][16][17][18], where different bosonic and fermionic theories can be related to each other by duality transformations. There are variations that consider more than one fermionic flavor [16,[19][20][21][22][23], as well as proposed extensions to 3+1 dimensions [24][25][26][27].…”
Section: Introductionmentioning
confidence: 99%
“…Some of these flows lead to supersymmetric fixed points where the bosonization duality [31][32][33][34] is related to the already well known Giveon-Kutasov duality [35][36][37]. 4 Recent computations have also investigated the duality in the Higgsed phase [38,39], finite temperature, background fields and additional flavors (see [40][41][42][43]). In particular, the puzzle of matching the dimensions of monopole operators [44] has led to the conjecture of the duality for finite N, κ [45].…”
mentioning
confidence: 99%