2,747 research outputs found

    Compact Simple Lie Groups and Their C-, S-, and E-Transforms

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    New continuous group transforms, together with their discretization over a lattice of any density and admissible symmetry, are defined for a general compact simple Lie groups of rank 2n<2\leq n<\infty. Rank 1 transforms are known. Rank 2 exposition of CC- and SS-transforms is in the literature. The EE-transforms appear here for the first time.Comment: Published in SIGMA (Symmetry, Integrability and Geometry: Methods and Applications) at http://www.emis.de/journals/SIGMA

    Orbit Functions

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    In the paper, properties of orbit functions are reviewed and further developed. Orbit functions on the Euclidean space EnE_n are symmetrized exponential functions. The symmetrization is fulfilled by a Weyl group corresponding to a Coxeter-Dynkin diagram. Properties of such functions will be described. An orbit function is the contribution to an irreducible character of a compact semisimple Lie group GG of rank nn from one of its Weyl group orbits. It is shown that values of orbit functions are repeated on copies of the fundamental domain FF of the affine Weyl group (determined by the initial Weyl group) in the entire Euclidean space EnE_n. Orbit functions are solutions of the corresponding Laplace equation in EnE_n, satisfying the Neumann condition on the boundary of FF. Orbit functions determine a symmetrized Fourier transform and a transform on a finite set of points.Comment: Published in SIGMA (Symmetry, Integrability and Geometry: Methods and Applications) at http://www.emis.de/journals/SIGMA

    Antisymmetric Orbit Functions

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    In the paper, properties of antisymmetric orbit functions are reviewed and further developed. Antisymmetric orbit functions on the Euclidean space EnE_n are antisymmetrized exponential functions. Antisymmetrization is fulfilled by a Weyl group, corresponding to a Coxeter-Dynkin diagram. Properties of such functions are described. These functions are closely related to irreducible characters of a compact semisimple Lie group GG of rank nn. Up to a sign, values of antisymmetric orbit functions are repeated on copies of the fundamental domain FF of the affine Weyl group (determined by the initial Weyl group) in the entire Euclidean space EnE_n. Antisymmetric orbit functions are solutions of the corresponding Laplace equation in EnE_n, vanishing on the boundary of the fundamental domain FF. Antisymmetric orbit functions determine a so-called antisymmetrized Fourier transform which is closely related to expansions of central functions in characters of irreducible representations of the group GG. They also determine a transform on a finite set of points of FF (the discrete antisymmetric orbit function transform). Symmetric and antisymmetric multivariate exponential, sine and cosine discrete transforms are given.Comment: Published in SIGMA (Symmetry, Integrability and Geometry: Methods and Applications) at http://www.emis.de/journals/SIGMA

    E-Orbit Functions

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    We review and further develop the theory of EE-orbit functions. They are functions on the Euclidean space EnE_n obtained from the multivariate exponential function by symmetrization by means of an even part WeW_{e} of a Weyl group WW, corresponding to a Coxeter-Dynkin diagram. Properties of such functions are described. They are closely related to symmetric and antisymmetric orbit functions which are received from exponential functions by symmetrization and antisymmetrization procedure by means of a Weyl group WW. The EE-orbit functions, determined by integral parameters, are invariant with respect to even part WeaffW^{\rm aff}_{e} of the affine Weyl group corresponding to WW. The EE-orbit functions determine a symmetrized Fourier transform, where these functions serve as a kernel of the transform. They also determine a transform on a finite set of points of the fundamental domain FeF^{e} of the group WeaffW^{\rm aff}_{e} (the discrete EE-orbit function transform).Comment: Published in SIGMA (Symmetry, Integrability and Geometry: Methods and Applications) at http://www.emis.de/journals/SIGMA

    Orthogonality within the Families of C-, S-, and E-Functions of Any Compact Semisimple Lie Group

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    The paper is about methods of discrete Fourier analysis in the context of Weyl group symmetry. Three families of class functions are defined on the maximal torus of each compact simply connected semisimple Lie group GG. Such functions can always be restricted without loss of information to a fundamental region Fˇ\check F of the affine Weyl group. The members of each family satisfy basic orthogonality relations when integrated over Fˇ\check F (continuous orthogonality). It is demonstrated that the functions also satisfy discrete orthogonality relations when summed up over a finite grid in Fˇ\check F (discrete orthogonality), arising as the set of points in Fˇ\check F representing the conjugacy classes of elements of a finite Abelian subgroup of the maximal torus T\mathbb T. The characters of the centre ZZ of the Lie group allow one to split functions ff on Fˇ\check F into a sum f=f1+...+fcf=f_1+...+f_c, where cc is the order of ZZ, and where the component functions fkf_k decompose into the series of CC-, or SS-, or EE-functions from one congruence class only.Comment: Published in SIGMA (Symmetry, Integrability and Geometry: Methods and Applications) at http://www.emis.de/journals/SIGMA

    Automorphisms of the fine grading of sl(n,C) associated with the generalized Pauli matrices

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    We consider the grading of sl(n,C)sl(n,\mathbb{C}) by the group Πn\Pi_n of generalized Pauli matrices. The grading decomposes the Lie algebra into n21n^2-1 one--dimensional subspaces. In the article we demonstrate that the normalizer of grading decomposition of sl(n,C)sl(n,\mathbb{C}) in Πn\Pi_n is the group SL(2,Zn)SL(2, \mathbb{Z}_n), where Zn\mathbb{Z}_n is the cyclic group of order nn. As an example we consider sl(3,C)sl(3,\mathbb{C}) graded by Π3\Pi_3 and all contractions preserving that grading. We show that the set of 48 quadratic equations for grading parameters splits into just two orbits of the normalizer of the grading in Π3\Pi_3
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