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Related papers: The Partition Function of ABJ Theory

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We study the BPS spectrum and vacuum moduli spaces in dimensional reductions of Chern-Simons-matter theories with N>=2 supersymmetry to zero dimensions. Our main example is a matrix model version of the ABJM theory which we relate…

High Energy Physics - Theory · Physics 2014-05-07 Joshua DeBellis , Richard J. Szabo

Conformal symmetry relates the metric on $AdS_2 \times S^{1}$ to that of $S^3$. This implies that under a suitable choice of boundary conditions for fields on $AdS_2$ the partition function of conformal field theories on these spaces must…

High Energy Physics - Theory · Physics 2017-04-05 Justin R. David , Edi Gava , Rajesh Kumar Gupta , Kumar Narain

Recently Aharony, Bergman and Jafferis (ABJ) have argued that a 3d U(N+M)xU(N) Chern-Simons gauge theory at level (k,-k) may have a vacuum with N=6 supersymmetry only if M<k+1 and if a certain period of the B-field in a IIA background is…

High Energy Physics - Theory · Physics 2009-12-15 Jarah Evslin , Stanislav Kuperstein

We consider the partition function of the superconformal Chern-Simons theories with the quiver diagram being the affine D-type Dynkin diagram. Rewriting the partition function into that of a Fermi gas system, we show that the perturbative…

High Energy Physics - Theory · Physics 2015-10-28 Sanefumi Moriyama , Tomoki Nosaka

We compute the supersymmetric partition function on L(r,1)xS^1, the lens space index, for 4d gauge theories related by supersymmetric dualities and involving non simply-connected groups. This computation is sensitive to the global…

High Energy Physics - Theory · Physics 2015-06-16 Shlomo S. Razamat , Brian Willett

We compute the supersymmetric partition function of the six-dimensional $(2,0)$ theory of type $A_{N-1}$ on $S^1 \times S^5$ in the presence of both codimension two and codimension four defects. We concentrate on a limit of the partition…

High Energy Physics - Theory · Physics 2016-04-28 Mathew Bullimore , Hee-Cheol Kim

We examine the three-dimensional N = 6 superconformal Chern--Simons theory with U(N) X U(N) gauge symmetry, which was recently constructed by Aharony, Bergman, Jafferis, and Maldacena (ABJM). Using a formulation with manifest SU(4)…

High Energy Physics - Theory · Physics 2009-02-20 Miguel A. Bandres , Arthur E. Lipstein , John H. Schwarz

It is known that the partition functions of the U(N) x U(N+M) ABJM theory satisfy a set of bilinear relations, which, written in the grand partition function, was recently found to be the q-Painleve III_3 equation. In this paper we have…

High Energy Physics - Theory · Physics 2021-08-06 Tomoki Nosaka

We clarify how mirror symmetry acts on 3d theories with N=2,3 or 4 supersymmetries and non-abelian Chern-Simons terms and then construct many new examples. We identify a new duality, geometric duality, that allows us to generate large…

High Energy Physics - Theory · Physics 2009-09-28 Kristan Jensen , Andreas Karch

We exactly compute the partition function for $U(2)_k\times U(2)_{-k}$ ABJM theory on $\mathbb S^3$ deformed by mass $m$ and Fayet-Iliopoulos parameter $\zeta $. For $k=1,2$, the partition function has an infinite number of Lee-Yang zeros.…

High Energy Physics - Theory · Physics 2016-01-27 Jorge G. Russo , Guillermo A. Silva

We consider a topological quiver matrix model which is expected to give a dual description of the instanton dynamics of topological U(N) gauge theory on D6 branes. The model is a higher dimensional analogue of the ADHM matrix model that…

High Energy Physics - Theory · Physics 2014-11-18 Hidetoshi Awata , Hiroaki Kanno

In this paper we will discuss non-anticommutative deformations of the harmonic superspace. We will analyse the non-anticommutative deformation of the superspace that break the supersymmetry from $\mathcal{N} =3$ supersymmetry to…

High Energy Physics - Theory · Physics 2015-06-12 Mir Faizal

We construct a generalized cusped Wilson loop operator in N = 6 super Chern-Simons-matter theories which is locally invariant under half of the supercharges. It depends on two parameters and interpolates smoothly between the 1/2 BPS line or…

High Energy Physics - Theory · Physics 2015-06-11 Luca Griguolo , Daniele Marmiroli , Gabriele Martelloni , Domenico Seminara

We argue the equivalence between the infrared conformal field theory of the 3d $\mathcal{N}=8$ supersymmetric Yang-Mills theories of ABCD ($U(N), SO(2N+1), Sp(2N), O(2N)$) gauge groups and the ABJ(M) theories of $U(N)_k\times U(\tilde…

High Energy Physics - Theory · Physics 2017-09-07 Dongmin Gang , Eunkyung Koh , Kimyeong Lee , Jaemo Park

We report on the exact computation of the S^3 partition function of U(N)_k\times U(N)_{-k} ABJM theory for k=1, N=1,...,19. The result is a polynomial in \pi^{-1} with rational coefficients. As an application of our results we numerically…

High Energy Physics - Theory · Physics 2012-10-31 Pavel Putrov , Masahito Yamazaki

This thesis delves into the $AdS_4/CFT_3$ correspondence (M-theory on $AdS_4 \times S^7 / \mathbb{Z}_k$ $\leftrightarrow$ ABJM theory) in a comprehensive and detailed manner. The ABJM theory i.e. $\mathcal{N} = 6$ $U(N)_k \times U(N)_{-k}$…

High Energy Physics - Theory · Physics 2024-08-23 Manikantt Mummalaneni

We propose an exact, finite $N$ formula for the partition function over $1/4^{th}$ BPS states in the conformal field theory on the world volume of $N$ coincident M5 branes and $1/8^{th}$ BPS states in the theory of $N$ coincident M2 branes.…

High Energy Physics - Theory · Physics 2009-09-29 Sayantani Bhattacharyya , Shiraz Minwalla

In this paper we will analyse the deformation of a ABJ theory in harmonic superspace. So, we will first discuss deformations of the harmonic superspace by a graviphoton background and then study the ABJ theory in this deformed harmonic…

High Energy Physics - Theory · Physics 2015-06-12 Mir Faizal

We use localization to compute the partition function of a four dimensional, supersymmetric, abelian gauge theory on a hemisphere coupled to charged matter on the boundary. Our theory has eight real supercharges in the bulk of which four…

High Energy Physics - Theory · Physics 2020-05-20 Rajesh Kumar Gupta , Christopher P. Herzog , Imtak Jeon

We discuss the N=2 superspace formulation of the N=8 superconformal Bagger-Lambert-Gustavsson theory, and of the N=6 superconformal Aharony-Bergman-Jafferis-Maldacena U(N)xU(N) Chern-Simons theory. In particular, we prove the full SU(4)…

High Energy Physics - Theory · Physics 2009-12-10 Marcus Benna , Igor Klebanov , Thomas Klose , Mikael Smedbäck