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In this article, we provide a comprehensive characterization of invariants of classical Lie superalgebras from the super-analog of the Schur-Weyl duality in a unified way. We establish $\mathfrak{g}$-invariants of the tensor algebra…

Representation Theory · Mathematics 2024-11-27 Yang Luo , Yongjie Wang

The Howe dual pair (sl(2),O(m)) allows the characterization of the classical Fourier transform (FT) on the space of rapidly decreasing functions as the exponential of a well-chosen element of sl(2) such that the Helmholtz relations are…

Classical Analysis and ODEs · Mathematics 2018-08-14 H. De Bie , R. Oste , J. Van der Jeugt

When the relative commutation relations between a set of m parafermions and n parabosons are of ``relative parafermion type'', the underlying algebraic structure is the classical orthosymplectic Lie superalgebra osp(2m+1|2n). The relative…

Mathematical Physics · Physics 2018-07-11 N. I. Stoilova , J. Van der Jeugt

We study the representation theory of the braids and ties algebra, or the $bt$-algebra, $ \cal E$. Using the cellular basis $\{m_{{\mathfrak s} {\mathfrak t}} \}$ for $ \cal E$ obtained in previous joint work with J. Espinoza we introduce…

Representation Theory · Mathematics 2021-11-15 Steen Ryom-Hansen

A Lagrangian of the topological field theory is found in the twisted osp(2|2)\oplus osp(2|2)conformal super algebra. The reduction on a moduli space is then elaborated through the vanishing Noether current.

High Energy Physics - Theory · Physics 2008-02-03 N. Ano

A bounded linear operator $U$ between Banach spaces is universal for the complement of some operator ideal $\mathfrak{J}$ if it is a member of the complement and it factors through every element of the complement of $\mathfrak{J}$. In the…

Functional Analysis · Mathematics 2017-11-28 Kevin Beanland , Ryan M. Causey

We define a class of orthosymplectic $osp(m;j|2n;\omega)$ and unitary $sl(m;j|n;\epsilon)$ superalgebras which may be obtained from $osp(m|2n)$ and $sl(m|n)$ by contractions and analytic continuations in a similar way as the special linear,…

High Energy Physics - Theory · Physics 2009-11-07 N. A. Gromov , I. V. Kostyakov , V. V. Kuratov

We construct real Jacobi forms with matrix index using path integrals. The path integral expressions represent elliptic genera of two-dimensional N=(2,2) supersymmetric theories. They arise in a family labeled by two integers N and k which…

High Energy Physics - Theory · Physics 2015-06-17 Sujay K. Ashok , Jan Troost

We extend our earlier work on the minimal unitary representation of $SO(d,2)$ and its deformations for $d=4,5$ and $6$ to arbitrary dimensions $d$. We show that there is a one-to-one correspondence between the minrep of $SO(d,2)$ and its…

High Energy Physics - Theory · Physics 2016-02-17 Sudarshan Fernando , Murat Gunaydin

We classify the finite-dimensional irreducible representations of the super Yangian associated with the orthosymplectic Lie superalgebra ${\frak osp}_{2|2n}$. The classification is given in terms of the highest weights and Drinfeld…

Representation Theory · Mathematics 2023-09-19 A. I. Molev

We provide a unified construction of the symplectic forms which arise in the solution of both N=2 supersymmetric Yang-Mills theories and soliton equations. Their phase spaces are Jacobian-type bundles over the leaves of a foliation in a…

High Energy Physics - Theory · Physics 2007-05-23 I. M. Krichever , D. H. Phong

Solvable Lie algebras having at least one Abelian descending central ideal are studied. It is shown that all such Lie algebras can be built up from canonically defined ideals. The nature of such ideals is elucidated and their construction…

Rings and Algebras · Mathematics 2021-02-15 R. García-Delgado , G. Salgado , O. A. Sánchez-Valenzuela

Throughout our work on the L\^e cycles of an affine hypersurface singularity, our primary algebraic tool consisted of a method for taking the Jacobian ideal of a complex analytic function and decomposing it into pure-dimensional "pieces".…

Algebraic Geometry · Mathematics 2007-05-23 David B. Massey

We prove an Amitsur-Levitzki type theorem for the Lie superalgebras osp(1,2n) inspired by Kostant's cohomological interpretation of the classical theorem. We show that the Lie superalgebras gl(p,q) cannot satisfy an Amitsur-Levitzki type…

Representation Theory · Mathematics 2009-11-10 Pierre-Alexandre Gie , Georges Pinczon , Rosane Ushirobira

A ladder structure of operators is presented for the Jacobi polynomials, J_n^(a,b)(x), with parameters n, a and b integers, showing that they are related to the unitary irreducible representation of SU(2,2) with quadratic Casimir…

Mathematical Physics · Physics 2013-07-30 E. Celeghini , M. A. del Olmo , M. A. Velasco

We introduce two subalgebras in the type A quantum affine algebra which are coideals with respect to the Hopf algebra structure. In the classical limit q -> 1 each subalgebra specializes to the enveloping algebra U(k), where k is a fixed…

Quantum Algebra · Mathematics 2009-11-07 A. I. Molev , E. Ragoucy , P. Sorba

We describe the minimal free resolution of the ideal of $2 \times 2$ subpermanents of a $2 \times n$ generic matrix $M$. In contrast to the case of $2 \times 2$ determinants, the $2 \times 2$ permanents define an ideal which is neither…

Commutative Algebra · Mathematics 2024-11-21 Fulvio Gesmundo , Hang , Huang , Hal Schenck , Jerzy Weyman

We solve the Killing-Yano equation on manifolds with a $G$-structure for $G=SO(n), U(n), SU(n), Sp(n)\cdot Sp(1), Sp(n), G_2$ and $Spin(7)$. Solutions include nearly-K\"ahler, weak holonomy $G_2$, balanced SU(n) and holonomy $G$ manifolds.…

High Energy Physics - Theory · Physics 2008-11-26 G. Papadopoulos

In this paper we reexamine the definition of parafermions and parabosons by means of Green's triple relations, and extend these relations by including a parity operator $P$ which is also determined by means of triple relations. As a…

Mathematical Physics · Physics 2026-05-01 N. I. Stoilova , J. Van der Jeugt

Let $\mathbb{S}$ denote the oscillatory module over the complex symplectic Lie algebra $\mathfrak{g}= \mathfrak{sp}(\mathbb{V}^{\mathbb{C}},\omega).$ Consider the $\mathfrak{g}$-module…

Representation Theory · Mathematics 2015-11-17 Svatopluk Krýsl
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