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Related papers: The Peter-Weyl Theorem for SU(1|1)

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We define a nonabelian version of particle-vortex duality, by dimensionally extending usual (1+1)-dimensional nonabelian T-duality to (2+1) dimensions. While we will explicitly describe a global $SU(2)$ symmetry, our methods can also be…

High Energy Physics - Theory · Physics 2016-09-21 Jeff Murugan , Horatiu Nastase

We define a notion of pseudo-unitarizability for weight modules over a generalized Weyl algebra (of rank one, with commutative coeffiecient ring $R$), which is assumed to carry an involution of the form $X^*=Y$, $R^*\subseteq R$. We prove…

Rings and Algebras · Mathematics 2012-10-26 Jonas T. Hartwig

We use the matrix model to describe the N=2 SO(N)/Sp(N) supersymmetric gauge theories with massive hypermultiplets in the fundamental representation. By taking the tree level superpotential perturbation made of a polynomial of a scalar…

High Energy Physics - Theory · Physics 2010-02-05 Changhyun Ahn , Soonkeon Nam

Using parafermionic field theoretical methods, the fundamentals of 2d fractional supersymmetry ${\bf Q}^{K} =P$ are set up. Known difficulties induced by methods based on the $U_{q}(sl(2))$ quantum group representations and non commutative…

High Energy Physics - Theory · Physics 2009-11-07 Ilham Benkaddour , El Hassane Saidi

Using the entropic inequalities for Shannon and Tsallis entropies new inequalities for some classical polynomials are obtained. To this end, an invertible mapping for the irreducible unitary representation of groups $SU(2)$ and $SU(1,1)$…

Quantum Physics · Physics 2015-11-24 V. I. Man'ko , L. A. Markovich

Let p > 2 be prime. We use purely local methods to determine the possible reductions of certain two-dimensional crystalline representations, which we call "pseudo-Barsotti-Tate representations", over arbitrary finite extensions of the…

Number Theory · Mathematics 2014-12-23 Toby Gee , Tong Liu , David Savitt

We study the generalized matrix model which corresponds to the n-point toric Virasoro conformal block. This describes four-dimensional N=2 SU(2)^n gauge theory with circular quiver diagram by the AGT relation. We first verify that it is…

High Energy Physics - Theory · Physics 2011-01-17 Kazunobu Maruyoshi , Futoshi Yagi

In this paper, we parametrize certain irreducible supercuspidal representations of U(1,1) and U(2) via explicit induction data. The parametrization depends on traceless elements of negative valuation in a quadratic extension of base field.…

Representation Theory · Mathematics 2008-11-25 Jitka Stehnova

We study the structure of an algebraic supergroup $\mathbb{G}$ and establish the Borel-Weil theorem for $\mathbb{G}$ to give a systematic construction of all simple supermodules over an arbitrary field. Especially when $\mathbb{G}$ has a…

Representation Theory · Mathematics 2020-11-17 Taiki Shibata

First and second fundamental theorems are given for polynomial invariants of a class of pseudo-reflection groups (including the Weyl groups of type $B_n$), under the assumption that the order of the group is invertible in the base field.…

Representation Theory · Mathematics 2015-02-12 M. Domokos

The projective superspace formulation for four-dimensional N = 2 matter-coupled supergravity presented in arXiv:0805.4683 makes use of the variant superspace realization for the N = 2 Weyl multiplet in which the structure group is SL(2,C) x…

High Energy Physics - Theory · Physics 2009-08-18 S. M. Kuzenko , U. Lindstrom , M. Rocek , G. Tartaglino-Mazzucchelli

In this paper, we study the theories with SU(2|4) symmetry which consist of the plane wave matrix model (PWMM), super Yang-Mills theory (SYM) on RxS^2 and SYM on RxS^3/Z_k. The last two theories can be realized as theories around particular…

High Energy Physics - Theory · Physics 2015-06-12 Yuhma Asano , Goro Ishiki , Takashi Okada , Shinji Shimasaki

In paper, we study the representation theory of super $W(2,2)$ algebra ${\mathfrak{L}}$. We prove that ${\mathfrak{L}}$ has no mixed irreducible modules and give the classification of irreducible modules of intermediate series. We…

Representation Theory · Mathematics 2017-05-29 Hao Wang , Huanxia Fa , Junbo Li

In this paper we obtain a decomposition formula of the uniform projection of the Weil character of a finite reductive dual pair consisting of a symplectic group and an even orthogonal group. This is the first and major step to give an…

Representation Theory · Mathematics 2020-08-03 Shu-Yen Pan

In N=1 supersymmetric SO(N)/USp(2N) gauge theories with the tree-level superpotential W(\Phi) that is an arbitrary polynomial of the adjoint matter \Phi, the massless fluctuations about each quantum vacuum are described by U(1)^n gauge…

High Energy Physics - Theory · Physics 2010-12-03 Changhyun Ahn , Yutaka Ookouchi

For semisimple Lie superalgebras over an algebraically closed field of characteristic zero, whose category of finite dimensional super representations is semisismple, we classify all irreducible super representations for which the…

Representation Theory · Mathematics 2010-02-24 T. Krämer , R. Weissauer

All finite dimensional irreducible representations of the simple Lie-Kac super algebra SU(2/1) are explicitly constructed in the Chevalley basis as complex matrices. For typical representations, the distinguished Dynkin label is not…

High Energy Physics - Theory · Physics 2022-07-15 Jean Thierry-Mieg , Peter D. Jarvis , Jerome Germoni

Let G be a split adjoint semisimple group over Q and K a maximal compact subgroup of the real points G(R). We shall give a uniform, short and essentially elementary proof of the Weyl law for cusp forms on congruence quotients of G(R)/K.…

Number Theory · Mathematics 2007-05-23 Elon Lindenstrauss , Akshay Venkatesh

The Seiberg-Witten curve and differential for ${\cal N}=2$ supersymmetric SU(N) gauge theory, with a massive hypermultiplet in the adjoint representation of the gauge group, are analyzed in terms of the elliptic Calogero-Moser integrable…

High Energy Physics - Theory · Physics 2009-10-30 Eric D'Hoker , D. H. Phong

An important problem from invariant theory is to describe the subspace of a tensor power of a representation invariant under the action of the group. According to Weyl's classic, the first main (later: 'fundamental') theorem of invariant…

Combinatorics · Mathematics 2015-04-13 Martin Rubey , Bruce W. Westbury
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