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We construct a new off-shell $\mathcal{N}{=}8$, $d{=}1$ nonlinear supermultiplet $(\mathbf{4,8,4})$ proceeding from the nonlinear realization of the $\mathcal{N}{=}8$, $d{=}1$ superconformal group $OSp(4^{\star}|4)$ in its supercoset…

High Energy Physics - Theory · Physics 2008-11-26 S. Bellucci , S. Krivonos , A. Marrani

In earlier work, Barchini, Kable, and Zierau constructed a number of conformally invariant systems of differential operators associated to Heisenberg parabolic subalgebras in simple Lie algebras. The construction was systematic, but the…

Representation Theory · Mathematics 2011-04-13 Toshihisa Kubo

We consider polynomial deformations of Lie superalgebras and their representations. For the class A(n-1,0) ~ sl(n/1), we identify families of superalgebras of quadratic and cubic type, consistent with Jacobi identities. For such deformed…

High Energy Physics - Theory · Physics 2011-06-30 Peter Jarvis

We describe the invariants for the coadjoint representation of all real Lie algebras with nontrivial Levi decomposition up to dimension eight.

Representation Theory · Mathematics 2007-05-23 Rutwig Campoamor-Stursberg

We define two new indecomposable (not fully reducible) ${\cal N}=8$, $d=1$ off-shell multiplets and consider the corresponding models of ${\cal N}=8$ supersymmetric mechanics with spin variables. Each multiplet is described off shell by a…

High Energy Physics - Theory · Physics 2026-01-22 Evgeny Ivanov , Stepan Sidorov

We define SU(2|1) supermultiplets described by chiral superfields having non-zero external spins with respect to SU(2) \subset SU(2|1) and show that their splitting into N=2, d=1 multiplets contains the so called "long" indecomposable N=2,…

High Energy Physics - Theory · Physics 2017-04-26 Evgeny Ivanov , Antonio Rivasplata Mendoza , Stepan Sidorov

We provide an explicit algorithm to calculate invariant tensors for the adjoint representation of the simple Lie algebra $sl(n)$, as well as arbitrary representation in terms of roots. We also obtain explicit formulae for the adjoint…

Geometric Topology · Mathematics 2007-05-23 R. Campoamor-Stursberg , V. O. Manturov

We give a survey of several models of irreducible complementary series representations and their limits, special representations, for the groups SU(n,1) and SO(n,1), including new ones. These groups, whose geometrical meaning is well known,…

Representation Theory · Mathematics 2007-05-23 M. I. Graev , A. M. Vershik

We prove that the scalar and $2\times 2$ matrix differential operators which preserve the simplest scalar and vector-valued polynomial modules in two variables have a fundamental Lie algebraic structure. Our approach is based on a general…

q-alg · Mathematics 2016-08-15 Federico Finkel , Niky Kamran

We prove an explicit formula for the invariant $\mu(\Lg)$ for finite-dimensional semisimple, and reductive Lie algebras $\Lg$ over $\C$. Here $\mu(\Lg)$ is the minimal dimension of a faithful linear representation of $\Lg$. The result can…

Representation Theory · Mathematics 2007-05-23 Dietrich Burde , Wolfgang Moens

For a simple real Lie group $G$ with Heisenberg parabolic subgroup $P$, we study the corresponding degenerate principal series representations. For a certain induction parameter the kernel of the conformally invariant system of second order…

Representation Theory · Mathematics 2024-04-25 Jan Frahm

We construct the non-minimal linear representations of the N=4 Extended Supersymmetry in one-dimension. They act on 8 bosonic and 8 fermionic fields. Inequivalent representations are specified by the mass-dimension of the fields and the…

High Energy Physics - Theory · Physics 2011-07-26 Marcelo Gonzales , Sadi Khodaee , Francesco Toppan

If $Q$ is a non degenerate quadratic form on ${\bb C}^n$, it is well known that the differential operators $X=Q(x)$, $Y=Q(\partial)$, and $H=E+\frac{n}{2}$, where $E$ is the Euler operator, generate a Lie algebra isomorphic to ${\go…

Representation Theory · Mathematics 2008-02-05 Hubert Rubenthaler

We study the minimal unitary representation (minrep) of SO(4,2) over an Hilbert space of functions of three variables, obtained by quantizing its quasiconformal action on a five dimensional space. The minrep of SO(4,2), which coincides with…

High Energy Physics - Theory · Physics 2015-05-14 Sudarshan Fernando , Murat Gunaydin

For the cases of irreducible representation, the complete set of operators necessary to specify uniquely the states. There are two ways of representing the state, using uncoupled and coupled basis. Here we discuss, how the number of…

Mathematical Physics · Physics 2007-05-23 Banibrata Mukhopadhyay , Subhadip Raychaudhuri

A general classification of linear differential and finite-difference operators possessing a finite-dimensional invariant subspace with a polynomial basis is given. The main result is that any operator with the above property must have a…

High Energy Physics - Theory · Physics 2008-02-03 Alexander Turbiner

We explicitly construct a finite number of discrete components in the restriction of complementary series representations of rank one semisimple groups $G$ to rank one subgroups $G_1$. For this we use the realizations of complementary…

Representation Theory · Mathematics 2016-04-06 Jan Möllers , Bent Ørsted , Genkai Zhang

Denote by $SL_3(\mathbb R)$ the special linear group of degree 3 over the real numbers, $A$ the subgroup consisting of the diagonal matrices with positive entries. In this paper, we study the algebraic and analytic properties of the…

Representation Theory · Mathematics 2025-09-09 Hanlong Fang , Xiaocheng Li , Yunfeng Zhang

We present a complete list of the dimension 8 operator basis in the standard model effective field theory using group theoretic techniques in a systematic and automated way. We adopt a new form of operators in terms of the irreducible…

High Energy Physics - Phenomenology · Physics 2021-07-28 Hao-Lin Li , Zhe Ren , Jing Shu , Ming-Lei Xiao , Jiang-Hao Yu , Yu-Hui Zheng

We determine the multiplicity of the irreducible representation V(n) of the simple Lie algebra sl(2,C) as a direct summand of its fourth exterior power $\Lambda^4 V(n)$. The multiplicity is 1 (resp. 2) if and only if n = 4, 6 (resp. n = 8,…

Rings and Algebras · Mathematics 2010-08-13 Murray R. Bremner , Hader A. elgendy