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ABJM theory as a Fermi gas
The partition function on the three-sphere of many supersymmetric Chern-Simons-matter theories reduces, by localization, to a matrix model. We develop a new method to study these models in the
From Weak to Strong Coupling in ABJM Theory
The partition function of $${\mathcal{N}=6}$$ supersymmetric Chern–Simons-matter theory (known as ABJM theory) on $${\mathbb{S}^3}$$ , as well as certain Wilson loop observables, are captured by a
Exact results in ABJM theory from topological strings
Recently, Kapustin, Willett and Yaakov have found, by using localization techniques, that vacuum expectation values of Wilson loops in ABJM theory can be calculated with a matrix model. We show that
Nonperturbative aspects of ABJM theory
A bstractUsing the matrix model which calculates the exact free energy of ABJM theory on $ {\mathbb{S}^3} $ we study non-perturbative effects in the large N expansion of this model, i.e., in the
BPS spectra and 3-manifold invariants
We provide a physical definition of new homological invariants $\mathcal{H}_a (M_3)$ of 3-manifolds (possibly, with knots) labeled by abelian flat connections. The physical system in question
Fivebranes and 3-manifold homology
A bstractMotivated by physical constructions of homological knot invariants, we study their analogs for closed 3-manifolds. We show that fivebrane compactifications provide a universal description of
EXACT ABJM PARTITION FUNCTION FROM TBA
We report on the exact computation of the S3 partition function of U(N)k × U(N)-k ABJM theory for k = 1, N = 1, …, 19. The result is a polynomial in π-1 with rational coefficients. As an application
Exact solutions of (0,2) Landau-Ginzburg models
In this paper we study the low energy physics of Landau-Ginzburg models with N $$ \mathcal{N} $$ = (0 , 2) supersymmetry. We exhibit a number of classes of relatively simple LG models where the
Large N duality beyond the genus expansion
We study non-perturbative aspects of the large N duality between Chern-Simons theory and topological strings, and we find a rich structure of large N phase transitions in the complex plane of the 't
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