Vector-Valued Polynomials and a Matrix Weight Function with B2-Action
The structure of orthogonal polynomials on $mathbb{R}^{2}$ with the weight function $vert x_{1}^{2}-x_{2}^{2}vert ^{2k_{0}}vertx_{1}x_{2}vert ^{2k_{1}}e^{-( x_{1}^{2}+x_{2}^{2})/2}$ is based on the Dunkl operators of type $B_{2}$. This refers to the full symmetry group of the square, generated by r...
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doaj-1dec57e00531476689e9cb835cde61422020-11-24T23:19:53ZengNational Academy of Science of UkraineSymmetry, Integrability and Geometry: Methods and Applications1815-06592013-01-019007Vector-Valued Polynomials and a Matrix Weight Function with B2-ActionCharles F. DunklThe structure of orthogonal polynomials on $mathbb{R}^{2}$ with the weight function $vert x_{1}^{2}-x_{2}^{2}vert ^{2k_{0}}vertx_{1}x_{2}vert ^{2k_{1}}e^{-( x_{1}^{2}+x_{2}^{2})/2}$ is based on the Dunkl operators of type $B_{2}$. This refers to the full symmetry group of the square, generated by reflections in the lines $x_{1}=0$ and $x_{1}-x_{2}=0$. The weight function is integrable if $k_{0},k_{1},k_{0} +k_{1}>-frac{1}{2}$. Dunkl operators can be defined for polynomials taking values in a module of the associated reflection group, that is, a vector space on which the group has an irreducible representation. The unique $2$-dimensional representation of the group $B_{2}$ is used here. The specific operators for this group and an analysis of the inner products on the harmonic vector-valued polynomials are presented in this paper. An orthogonal basis for the harmonic polynomials is constructed, and is used to define an exponential-type kernel. In contrast to the ordinary scalar case the inner product structure is positive only when $( k_{0},k_{1})$ satisfy $-frac{1}{2} < k_{0}pm k_{1} < frac{1}{2}$. For vector polynomials $(f_{i})_{i=1}^{2}$, $(g_{i})_{i=1}^{2}$ the inner product has the form $iint_{mathbb{R}^{2}}f(x) K(x) g(x)^{T}e^{-( x_{1}^{2}+x_{2}^{2})/2}dx_{1}dx_{2}$ where the matrix function $K(x)$ has to satisfy various transformation and boundary conditions. The matrix $K$ is expressed in terms of hypergeometric functions.http://dx.doi.org/10.3842/SIGMA.2013.007matrix Gaussian weight functionharmonic polynomials |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Charles F. Dunkl |
spellingShingle |
Charles F. Dunkl Vector-Valued Polynomials and a Matrix Weight Function with B2-Action Symmetry, Integrability and Geometry: Methods and Applications matrix Gaussian weight function harmonic polynomials |
author_facet |
Charles F. Dunkl |
author_sort |
Charles F. Dunkl |
title |
Vector-Valued Polynomials and a Matrix Weight Function with B2-Action |
title_short |
Vector-Valued Polynomials and a Matrix Weight Function with B2-Action |
title_full |
Vector-Valued Polynomials and a Matrix Weight Function with B2-Action |
title_fullStr |
Vector-Valued Polynomials and a Matrix Weight Function with B2-Action |
title_full_unstemmed |
Vector-Valued Polynomials and a Matrix Weight Function with B2-Action |
title_sort |
vector-valued polynomials and a matrix weight function with b2-action |
publisher |
National Academy of Science of Ukraine |
series |
Symmetry, Integrability and Geometry: Methods and Applications |
issn |
1815-0659 |
publishDate |
2013-01-01 |
description |
The structure of orthogonal polynomials on $mathbb{R}^{2}$ with the weight function $vert x_{1}^{2}-x_{2}^{2}vert ^{2k_{0}}vertx_{1}x_{2}vert ^{2k_{1}}e^{-( x_{1}^{2}+x_{2}^{2})/2}$ is based on the Dunkl operators of type $B_{2}$. This refers to the full symmetry group of the square, generated by reflections in the lines $x_{1}=0$ and $x_{1}-x_{2}=0$. The weight function is integrable if $k_{0},k_{1},k_{0} +k_{1}>-frac{1}{2}$. Dunkl operators can be defined for polynomials taking values in a module of the associated reflection group, that is, a vector space on which the group has an irreducible representation. The unique $2$-dimensional representation of the group $B_{2}$ is used here. The specific operators for this group and an analysis of the inner products on the harmonic vector-valued polynomials are presented in this paper. An orthogonal basis for the harmonic polynomials is constructed, and is used to define an exponential-type kernel. In contrast to the ordinary scalar case the inner product structure is positive only when $( k_{0},k_{1})$ satisfy $-frac{1}{2} < k_{0}pm k_{1} < frac{1}{2}$. For vector polynomials $(f_{i})_{i=1}^{2}$, $(g_{i})_{i=1}^{2}$ the inner product has the form $iint_{mathbb{R}^{2}}f(x) K(x) g(x)^{T}e^{-( x_{1}^{2}+x_{2}^{2})/2}dx_{1}dx_{2}$ where the matrix function $K(x)$ has to satisfy various transformation and boundary conditions. The matrix $K$ is expressed in terms of hypergeometric functions. |
topic |
matrix Gaussian weight function harmonic polynomials |
url |
http://dx.doi.org/10.3842/SIGMA.2013.007 |
work_keys_str_mv |
AT charlesfdunkl vectorvaluedpolynomialsandamatrixweightfunctionwithb2action |
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