q-Deformed Euclidean algebras and their representations

A new q-deformed Euclidean algebra U_q (iso _n ), based on a definition of the algebra U_q (so _n ) different from the Drinfeld-Jimbo definition, is given. Infinite-dimensional representations T_a of this algebra, characterized by one complex number, is described. Explicit formulas for operators of these representations in an orthonormal basis are derived. The spectrum of the operator T_a(I_n) corresponding to a q-analogue of the infinitesimal operator of shifts along the n-th axis is given. Contrary to the case of the classical Euclidean algebraiso _n, this spectrum is discrete and the spectrum points have one point of accumulation.Translated from Teoreticheskaya i Matematicheskaya Fizika, Vol. 103, No. 3, pp. 467–475, June, 1995.     

An Algorithm for Computing the Global Basis of a Finite Dimensional Irreducible U q ( so 2 n + 1 ) or U q ( so 2 n )-Module

Abstract

We describe a simple algorithm for computing the canonical basis of any irreducible finite-dimensional U _q (s o _2n+1) or U _q (s o _2n )-module.     

Representations of the Quantum Algebra Uq(un, 1)

The main aim of the paper is to study infinite-dimensional representations of the real form U _q (u _{n, 1}) of the quantized universal enveloping algebra U _q (gl _{n + 1}). We investigate the principal series of representations of U _q (u _{n, 1}) and calculate the intertwining operators for pairs of these representations. Some of the principal series representations are reducible. The structure of these representations is determined. Then we classify irreducible representations of U _q (u _{n, 1}) obtained from irreducible and reducible principal series representations. All *-representations in this set of irreducible representations are separated. Unlike the classical case, the algebra U _q (u _{n, 1}) has finite-dimensional irreducible *-representations.     

Matching Realization of Uq（sln＋1） of Higher Rank in the Quantum Weyl Algebra Wq（2n）

In the paper, we further realize the higher rank quantized universal enveloping algebra Uq（sln＋1） as certain quantum differential operators in the quantum Weyl algebra Wq （2n） defined over the quantum divided power algebra Sq（n） of rank n. We give the quantum differential operators realization for both the simple root vectors and the non-simple root vectors of Uq（sln＋1）. The nice behavior of the quantum root vectors formulas under the action of the Lusztig symmetries once again indicates that our realization model is naturally matched.     

Orthosymplectic Quantum Function Superalgebras OSPq（2l＋ 1｜2n）

By the R-matrix of orthosymplectic quantum superalgebra U _q (osp(2l+1|2n)) in the vector representation, we establish the corresponding quantum Hopf superalgebra OSP _q (2l + 1|2n). Furthermore, it is shown that OSP _q (2l + 1|2n) is coquasitriangular.     

Leonard Pairs and Leonard Triples of q-Racah Type from the Quantum Algebra U q (sl 2)

In this article, we describe the construction of Leonard pairs and Leonard triples that have q-Racah type from U _q (sl ₂)-modules by using equitable generators of U _q (sl ₂). Our result solves an open problem proposed by Terwilliger.     

U(n) Wigner coefficients,the path sum formula,and invariant G-functions

We prove the path sum formula for computing the U(n) invariant denominator functions associated to stretched U(n) Wigner operators. A family of U(n) invariant polynomials G_[λ]⁽ⁿ⁾ is then defined which generalize the _μG_q⁽ⁿ⁾ polynomials previously studied. The G_[λ]⁽ⁿ⁾ polynomials are shown to satisfy a number of difference equations and have symmetry properties similar to the _μG_q⁽ⁿ⁾ polynomials. We also give a direct proof of the important transposition symmetry for the G_[λ]⁽ⁿ⁾ polynomials. To enable the non-specialist to understand the foundations for these remarkable polynomials, we provide an exposition of the boson calculus and the construction of the multiplicity-free U(n) Wigner operators.     

Embeddings of Un(q2) and symmetric strongly regular graphs

In the geometric setting of the embedding of the unitary group U_n(q²) inside an orthogonal or a symplectic group over the subfield GF(q) of GF(q²), q odd, we show the existence of infinite families of transitive two‐character sets with respect to hyperplanes that in turn define new symmetric strongly regular graphs and two‐weight codes. © 2009 Wiley Periodicals, Inc. J Combin Designs 18: 248–253, 2010     

Partition models for the crystal of the basic $U_{q}(\widehat {\mathfrak{sl}}_{n})$-module

For each n ≥3, we construct an uncountable family of models of the crystal of the basic U_q([^(\mathfrak sl)]_n)U_{q}(\widehat {\mathfrak {sl}}_{n})-module. These models are all based on partitions, and include the usual n-regular and n-restricted models, as well as Berg’s ladder crystal, as special cases.     

An algebraic characterization of sets of type (0,n)1 inAG(2,q)

In this paper we prove that inAG(2,q) a set of type (0,n)₁ exists if and only if an algebraic systemS admits solutions inGF(q ²).     

q-Difference intertwining operators and q-conformal invariant equations

We first recall a canonical procedure for the construction of the invariant differential operators and equations for arbitrary complex or real noncompact semisimple Lie groups. Then we present the application of this procedure to the case of quantum groups. In detail is given the construction of representations of the quantum algebra U _q (sl(n)) labelled by n–1 complex numbers and acting in the spaces of functions of n(n–1)/2 noncommuting variables, which generate a q-deformed SL(4) flag manifold. The conditions for reducibility of these representations and the procedure for the construction of the q-difference intertwining operators are given. Using these results for the case n=4 we propose infinite hierarchies of q-difference equations which are q-conformal invariant. The lowest member of one of these hierarchies are new q-Maxwell equations. We propose also new q-Minkowski spacetime which is part of a q-deformed SU(2,2) flag manifold.     

Quantum superdeterminants for OSP q (1-2n)

It is shown that there exists a quantum superdeterminant sdet _q T for the quantum super group OSP _q (1|2n). It is also shown that the quantum superdeterminant sdet _q T is a group-like element and central, and that the square of sdet _q T for OSP _q (1|2n) is equal to 1.     

Crystal Bases and Monomials for U q (G 2)-Modules

In this article, we give a new realization of crystal bases for irreducible highest weight modules over U _q (G ₂) in terms of monomials. We also discuss the natural connection between the monomial realization and tableau realization.

Communicated by K. Misra     

The number of connected sparsely edged graphs. II. Smooth graphs and blocks

A smooth graph is a connected graph without endpoints; f(n, q) is the number of connected graphs, v(n, q) is the number of smooth graphs, and u(n, q) is the number of blocks on n labeled points and q edges: W_k, V_k, and U_k are the exponential generating functions of f(n, n + k), v(n, n + k), and u(n, n + k), respectively. For any k ? 1, our reduction method shows that V_k can be deduced at once from W_k, which was found for successive k by the computer method described in our previous paper. Again the reduction method shows that U_k must be a sum of powers (mostly negative) of 1 - X and, given this information, we develop a recurrence method well suited to calculate U_k for successive k. Exact formulas for v(n, n + k) and u(n, n + k) for general n follow at once.     

A Morita equivalence theorem for Hecke algebra ℋq(Dn) when n is even

 In this paper we prove a Morita equivalence theorem for Hecke algebras of type D _n when n is even, which generalize a similar result obtained by C. Pallikaros ([P, (3.7)]) when n is odd. As a consequence, we construct all the irreducible ℋ _q (D _n )-modules when f _n (q)≠ 0 (see [P, (2.12)] for definition of f _n (q)) and show that ℋ _q (D _n ) is split in this case. Received: 19 February 2001 / Revised version: 26 January 2002     

On the centers of quantum groups of <Emphasis Type="Italic">A</Emphasis><Subscript><Emphasis Type="Italic">n</Emphasis></Subscript>-type

Let g be the finite dimensional simple Lie algebra of type An, and let U? = U _q (g,Λ) and U = U _q (g,Q) be the quantum groups defined over the weight lattice and over the root lattice, respectively. In this paper, we find two algebraically independent central elements in U? for all n ≥ 2 and give an explicit formula of the Casimir elements for the quantum group U? = U _q (g,Λ), which corresponds to the Casimir element of the enveloping algebra U(g). Moreover, for n = 2 we give explicitly generators of the center subalgebras of the quantum groups U? = U _q (g,Λ) and U = U _q (g,Q).     

Decomposition ofq-deformed Fock spaces

A decomposition of the level-oneq-deformed Fock space representations ofU _q(sl _n ) is given. It is found that the action ofU _q(sl _n ) on these Fock spaces is centralized by a Heisenberg algebra, which arises from the center of the affine Hecke algebra _N in the limitN . Theq-deformed Fock space is shown to be isomorphic as aU _q(sl _n )-Heisenberg-bimodule to the tensor product of a level-one irreducible highest weight representation ofU _q(sl _n ) and the Fock representation of the Heisenberg algebra. The isomorphism is used to decompose theq-wedging operators, which are intertwiners between theq-deformed Fock spaces, into constituents coming fromU _q(sl _n ) and from the Heisenberg algebra.     

Unipotent Conjugacy in General Linear Groups

Let U(n,q) be the group of upper uni-triangular matrices in GL(n,q), the n-dimensional general linear group over the field of q elements. The number of U(n,q)-conjugacy classes in GL(n,q) is, as a function of q, for fixed n, a polynomial in q with integral coefficients.     

Reflection equation algebras, coideal subalgebras, and their centres

Reflection equation algebras and related U_q(\mathfrak g){U{_q}(\mathfrak g)} -comodule algebras appear in various constructions of quantum homogeneous spaces and can be obtained via transmutation or equivalently via twisting by a cocycle. In this paper we investigate algebraic and representation theoretic properties of such so called ‘covariantized’ algebras, in particular concerning their centres, invariants, and characters. The locally finite part F_l(U_q (\mathfrak g)){F_l(U{_q} (\mathfrak g))} of U_q(\mathfrak g){U{_q}(\mathfrak g)} with respect to the left adjoint action is a special example of a covariantized algebra. Generalising Noumi’s construction of quantum symmetric pairs we define a coideal subalgebra B _f of U_q(\mathfrak g){U{_q}(\mathfrak g)} for each character f of a covariantized algebra. We show that for any character f of F_l(U_q(\mathfrak g)){F_l(U{_q}(\mathfrak g))} the centre Z(B _f ) canonically contains the representation ring Rep(\mathfrak g){{\rm Rep}(\mathfrak g)} of the semisimple Lie algebra \mathfrak g{\mathfrak g} . We show moreover that for \mathfrak g = \mathfrak sl_n(\mathbb C){\mathfrak g = {\mathfrak sl}_n(\mathbb C)} such characters can be constructed from any invertible solution of the reflection equation and hence we obtain many new explicit realisations of Rep(\mathfrak sl_n(\mathbb C)){{\rm Rep}({\mathfrak sl}_n(\mathbb C))} inside U_q(\mathfrak sl_n(\mathbb C)){U_q({\mathfrak sl}_n(\mathbb C))} . As an example we discuss the solutions of the reflection equation corresponding to the Grassmannian manifold Gr(m,2m) of m-dimensional subspaces in \mathbb C^2m{{\mathbb C}^{2m}}.     

LatticeW algebras and quantum groups

We present Feigin's construction [Lectures given in Landau Institute] of latticeW algebras and give some simple results: lattice Virasoro andW ₃ algebras. For the simplest caseg=sl(2), we introduce the wholeU _q(2)) quantum group on this lattice. We find the simplest two-dimensional module as well as the exchange relations and define the lattice Virasoro algebra as the algebra of invariants ofU _q(sl(2)). Another generalization is connected with the lattice integrals of motion as the invariants of the quantum affine groupU _q(ñ₊). We show that Volkov's scheme leads to a system of difference equations for a function of non-commutative variables.Landau Institute for Theoretical Physics, 142432, Chernogolovka, Russia. Published in Teoreticheskaya i Matematicheskaya Fizika, Vol. 100, No. 1, pp. 132–147, July, 1994.