$${\mathcal{N} = 2}$$ N = 2 Supersymmetric AdS4 Solutions of M-theory
نویسندگان
چکیده
منابع مشابه
Upper bounds on the solutions to n = p+m^2
ardy and Littlewood conjectured that every large integer $n$ that is not a square is the sum of a prime and a square. They believed that the number $mathcal{R}(n)$ of such representations for $n = p+m^2$ is asymptotically given by begin{equation*} mathcal{R}(n) sim frac{sqrt{n}}{log n}prod_{p=3}^{infty}left(1-frac{1}{p-1}left(frac{n}{p}right)right), end{equation*} where $p$ is a prime, $m$ is a...
متن کاملN = 2 supersymmetric Yang-Mills Theory
In this final project, we will report our understanding of Seiberg Witten theory [1][2]. The low energy effective theory of N = 2 supersymmetric Yang-mill theory has a non-trivial quantum moduli space. And the structure of the moduli space can be exactly determined by the property near the singularities of the moduli space. This theory also provide a example for electric-magnetic duality. In th...
متن کاملN = 2 Supersymmetric Yang-Mills Theory
The first part of this paper is primarily devoted to the construction of the N = 2 supersymmetric Lagrangians with both gauge multiplets and matter multiplets from the N = 1 superfields and Lagrangians. While in the second part we describe the Seiberg-Witten analysis of the N = 2 pure SU(2) gauge theory. We discuss the parametrization of the moduli space and the breaking of R-symmetries, and th...
متن کاملupper bounds on the solutions to n = p+m^2
ardy and littlewood conjectured that every large integer $n$ that is not a square is the sum of a prime and a square. they believed that the number $mathcal{r}(n)$ of such representations for $n = p+m^2$ is asymptotically given by begin{equation*} mathcal{r}(n) sim frac{sqrt{n}}{log n}prod_{p=3}^{infty}left(1-frac{1}{p-1}left(frac{n}{p}right)right), end{equation*} where $p$ is a prime, $m$ is a...
متن کاملNon - anticommutative N = 2 Supersymmetric SU ( 2 ) Gauge Theory 1
We calculate the component Lagrangian of the four-dimensional non-anticommutative (with a singlet deformation parameter) and fully N=2 supersymmetric gauge field theory with the simple gauge group SU(2). We find that the deformed (classical) scalar potential is unbounded from below, in contrast to the undeformed case. Supported in part by the JSPS and the Volkswagen Stiftung Email address: keto...
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ژورنال
عنوان ژورنال: Communications in Mathematical Physics
سال: 2013
ISSN: 0010-3616,1432-0916
DOI: 10.1007/s00220-013-1865-0