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Given a semidirect product $\frak{g}=\frak{s}\uplus\frak{r}$ of semisimple Lie algebras $\frak{s}$ and solvable algebras $\frak{r}$, we construct polynomial operators in the enveloping algebra $\mathcal{U}(\frak{g})$ of $\frak{g}$ that…

Mathematical Physics · Physics 2009-11-13 R. Campoamor-Stursberg , S. G. Low

A novel invariant decomposition of diagonalizable $n \times n$ matrices into $n$ commuting matrices is presented. This decomposition is subsequently used to split the fundamental representation of $\mathfrak{su}(3)$ Lie algebra elements…

Mathematical Physics · Physics 2025-10-16 Martin Roelfs

When the parameter of deformation q is a m-th root of unity, the centre of U_q(sl(N))$ contains, besides the usual q-deformed Casimirs, a set of new generators, which are basically the m-th powers of all the Cartan generators of U_q(sl(N)).…

High Energy Physics - Theory · Physics 2009-10-22 Daniel Arnaudon , Michel Bauer

For two different natural definitions of Casimir operators for simple Lie algebras we show that their eigenvalues in the adjoint representation can be expressed polynomially in the universal Vogel's parameters $\alpha, \beta, \gamma$ and…

Representation Theory · Mathematics 2015-05-28 R. L. Mkrtchyan , A. N. Sergeev , A. P. Veselov

The Askey-Wilson algebra is realized in terms of the elements of the quantum algebras $U_q(\mathfrak{su}(2))$ or $U_q(\mathfrak{su}(1,1))$. A new realization of the Racah algebra in terms of the Lie algebras $\mathfrak{su}(2)$ or…

Quantum Algebra · Mathematics 2020-10-09 Nicolas Crampe , Dounia Shaaban Kabakibo , Luc Vinet

For various series of complex semi-simple Lie algebras $\fg (t)$ equipped with irreducible representations $V(t)$, we decompose the tensor powers of $V(t)$ into irreducible factors in a uniform manner, using a tool we call {\it diagram…

Algebraic Geometry · Mathematics 2007-05-23 J. M. Landsberg , L. Manivel

In this paper we prove that every irreducible representation of a Leibniz algebra can be obtained from irreducible representations of the semisimple Lie algebra from the Levi decomposition. We also prove that - in general - for (semi)simple…

Representation Theory · Mathematics 2015-02-26 Fialowski Alice , Mihálka Éva Zsuzsanna

We compute the matrix elements of $SO(3)$ in any finite-dimensional irreducible representation of $sl_3$. They are expressed in terms of a double sum of products of Krawtchouk and Racah polynomials which generalize the Griffiths-Krawtchouk…

Representation Theory · Mathematics 2024-07-25 Nicolas Crampe , Julien Gaboriaud , Loïc Poulain d'Andecy , Luc Vinet

We show that any semi-direct sum $L$ of Lie algebras with Levi factor $S$ must be perfect if the representation associated with it does not possess a copy of the trivial representation. As a consequence, all invariant functions of $L$ must…

Differential Geometry · Mathematics 2023-01-04 J C Ndogmo

It is shown that the $\mathfrak{gl}(3)$ polynomial integrable system, introduced by Sokolov-Turbiner in [arXiv:1409.7439], is equivalent to the $\mathfrak{gl}(3)$ quantum Euler-Arnold top in a constant magnetic field. Their Hamiltonian as…

Mathematical Physics · Physics 2025-03-10 Alexander V. Turbiner , Juan Carlos Lopez Vieyra , Miguel Ayala

We present a new look at description of real finite-dimensional Lie algebras. The basic element turns out to be a pair $(F,v)$ consisting of a linear mapping $F\in End(V)$ and its eigenvector $v$. This pair allows to build a Lie bracket on…

Mathematical Physics · Physics 2023-05-05 Alina Dobrogowska , Grzegorz Jakimowicz

The irreducible representations of two intermediate Casimir elements associated to the recoupling of three identical irreducible representations of $U_q(\mathfrak{sl}_2)$ are considered. It is shown that these intermediate Casimirs are…

Representation Theory · Mathematics 2021-08-31 Nicolas Crampé , Luc Vinet , Meri Zaimi

Let $K$ be an arbitrary field of characteristic zero and $A$ a commutative associative $ K$-algebra which is an integral domain. Denote by $R$ the fraction field of $A$ and by $W(A)=RDer_{\mathbb K}A,$ the Lie algebra of $\mathbb…

Rings and Algebras · Mathematics 2016-08-11 A. P. Petravchuk

We show that $\frak{su}(2)$ Lie algebras of coordinate operators related to quantum spaces with $\frak{su}(2)$ noncommutativity can be conveniently represented by $SO(3)$-covariant poly-differential involutive representations. We show that…

High Energy Physics - Theory · Physics 2017-08-22 Tajron Jurić , Timothé Poulain , Jean-Christophe Wallet

We give a general method to construct a complete set of linearly independent Casimir operators of a Lie algebra with rank N. For a Casimir operator of degree p, this will be provided by an explicit calculation of its symmetric coefficients…

High Energy Physics - Theory · Physics 2009-10-30 H. R. Karadayi , M. Gungormez

By a theorem of D. Wigner, an irreducible unitary representation with non-zero $(\frak{g},K)$-cohomology has trivial infinitesimal character, and hence up to unitary equivalence, these are finite in number. We have determined the number of…

Representation Theory · Mathematics 2023-09-25 Ankita Pal , Pampa Paul

We present the most general polynomial Lie algebra generated by a second order integral of motion and one of order M, construct the Casimir operator, and show how the Jacobi identity provides the existence of a realization in terms of…

Mathematical Physics · Physics 2015-06-18 Phillip S. Isaac , Ian Marquette

We describe properties of the nonstandard q-deformation U'_q(so_n) of the universal enveloping algebra U(so_n) of the Lie algebra so_n which does not coincide with the Drinfeld--Jimbo quantum algebra U_q(so_n). In particular, it is shown…

Quantum Algebra · Mathematics 2007-05-23 N. Z. Iorgov , A. U. Klimyk

We construct characteristic identities for the split (polarized) Casimir operators of the simple Lie algebras in adjoint representation. By means of these characteristic identities, for all simple Lie algebras we derive explicit formulae…

Mathematical Physics · Physics 2021-06-10 A. P. Isaev , S. O. Krivonos

Representations of $SO(5)_{q}$ are constructed explicitly on the Chevalley basis for all $q$, generic and root of unity. Matrix elements of the generators are obtained for all representations depending on three variable indices, the maximal…

High Energy Physics - Theory · Physics 2007-05-23 Amitabha Chakrabarti